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Author name code: heinzel
ADS astronomy entries on 2022-09-14
author:"Heinzel, Petr" 

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Title: Coronal mass ejection followed by a prominence eruption and
    a plasma blob as observed by Solar Orbiter
Authors: Bemporad, A.; Andretta, V.; Susino, R.; Mancuso, S.; Spadaro,
   D.; Mierla, M.; Berghmans, D.; D'Huys, E.; Zhukov, A. N.; Talpeanu,
   D. -C.; Colaninno, R.; Hess, P.; Koza, J.; Jejčič, S.; Heinzel,
   P.; Antonucci, E.; Da Deppo, V.; Fineschi, S.; Frassati, F.; Jerse,
   G.; Landini, F.; Naletto, G.; Nicolini, G.; Pancrazzi, M.; Romoli,
   M.; Sasso, C.; Slemer, A.; Stangalini, M.; Teriaca, L.
2022A&A...665A...7B    Altcode: 2022arXiv220210294B
  Context. On 2021 February 12, two subsequent eruptions occurred above
  the western limb of the Sun, as seen along the Sun-Earth line. The
  first event was a typical slow coronal mass ejection (CME), followed
  ∼7 h later by a smaller and collimated prominence eruption,
  originating south of the CME, followed by a plasma blob. These
  events were observed not only by the SOHO and STEREO-A missions,
  but also by the suite of remote-sensing instruments on board Solar
  Orbiter. <BR /> Aims: We show how data acquired by the Full Sun
  Imager (FSI), the Metis coronagraph, and the Heliospheric Imager
  (HI) from the Solar Orbiter perspective can be combined to study
  the eruptions and different source regions. Moreover, we show how
  Metis data can be analyzed to provide new information about solar
  eruptions. <BR /> Methods: Different 3D reconstruction methods were
  applied to the data acquired by different spacecraft, including
  remote-sensing instruments on board Solar Orbiter. Images acquired
  by the two Metis channels in the visible light (VL) and H I Ly-α
  line (UV) were combined to derive physical information about the
  expanding plasma. The polarization ratio technique was also applied
  for the first time to Metis images acquired in the VL channel. <BR
  /> Results: The two eruptions were followed in 3D from their source
  region to their expansion in the intermediate corona. By combining
  VL and UV Metis data, the formation of a post-CME current sheet (CS)
  was followed for the first time in the intermediate corona. The
  plasma temperature gradient across a post-CME blob propagating
  along the CS was also measured for the first time. Application
  of the polarization ratio technique to Metis data shows that by
  combining four different polarization measurements, the errors are
  reduced by ∼5 − 7%. This constrains the 3D plasma distribution
  better. <P />Movies associated to Figs. 4-7 are available at <A
  href="https://www.aanda.org/10.1051/0004-6361/202243162/olm">https://www.aanda.org</A>

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Title: Linking Small-scale Solar Wind Properties with Large-scale
    Coronal Source Regions through Joint Parker Solar Probe-Metis/Solar
    Orbiter Observations
Authors: Telloni, Daniele; Zank, Gary P.; Sorriso-Valvo, Luca;
   D'Amicis, Raffaella; Panasenco, Olga; Susino, Roberto; Bruno, Roberto;
   Perrone, Denise; Adhikari, Laxman; Liang, Haoming; Nakanotani, Masaru;
   Zhao, Lingling; Hadid, Lina Z.; Sánchez-Cano, Beatriz; Verscharen,
   Daniel; Velli, Marco; Grimani, Catia; Marino, Raffaele; Carbone,
   Francesco; Mancuso, Salvatore; Biondo, Ruggero; Pagano, Paolo; Reale,
   Fabio; Bale, Stuart D.; Kasper, Justin C.; Case, Anthony W.; de Wit,
   Thierry Dudok; Goetz, Keith; Harvey, Peter R.; Korreck, Kelly E.;
   Larson, Davin; Livi, Roberto; MacDowall, Robert J.; Malaspina, David
   M.; Pulupa, Marc; Stevens, Michael L.; Whittlesey, Phyllis; Romoli,
   Marco; Andretta, Vincenzo; Deppo, Vania Da; Fineschi, Silvano; Heinzel,
   Petr; Moses, John D.; Naletto, Giampiero; Nicolini, Gianalfredo;
   Spadaro, Daniele; Stangalini, Marco; Teriaca, Luca; Capobianco,
   Gerardo; Capuano, Giuseppe E.; Casini, Chiara; Casti, Marta; Chioetto,
   Paolo; Corso, Alain J.; Leo, Yara De; Fabi, Michele; Frassati,
   Federica; Frassetto, Fabio; Giordano, Silvio; Guglielmino, Salvo L.;
   Jerse, Giovanna; Landini, Federico; Liberatore, Alessandro; Magli,
   Enrico; Massone, Giuseppe; Messerotti, Mauro; Pancrazzi, Maurizio;
   Pelizzo, Maria G.; Romano, Paolo; Sasso, Clementina; Schühle, Udo;
   Slemer, Alessandra; Straus, Thomas; Uslenghi, Michela; Volpicelli,
   Cosimo A.; Zangrilli, Luca; Zuppella, Paola; Abbo, Lucia; Auchère,
   Frédéric; Cuadrado, Regina Aznar; Berlicki, Arkadiusz; Ciaravella,
   Angela; Lamy, Philippe; Lanzafame, Alessandro; Malvezzi, Marco;
   Nicolosi, Piergiorgio; Nisticò, Giuseppe; Peter, Hardi; Solanki,
   Sami K.; Strachan, Leonard; Tsinganos, Kanaris; Ventura, Rita; Vial,
   Jean-Claude; Woch, Joachim; Zimbardo, Gaetano
2022ApJ...935..112T    Altcode:
  The solar wind measured in situ by Parker Solar Probe in the very
  inner heliosphere is studied in combination with the remote-sensing
  observation of the coronal source region provided by the METIS
  coronagraph aboard Solar Orbiter. The coronal outflows observed near
  the ecliptic by Metis on 2021 January 17 at 16:30 UT, between 3.5 and
  6.3 R <SUB>⊙</SUB> above the eastern solar limb, can be associated
  with the streams sampled by PSP at 0.11 and 0.26 au from the Sun,
  in two time intervals almost 5 days apart. The two plasma flows
  come from two distinct source regions, characterized by different
  magnetic field polarity and intensity at the coronal base. It follows
  that both the global and local properties of the two streams are
  different. Specifically, the solar wind emanating from the stronger
  magnetic field region has a lower bulk flux density, as expected,
  and is in a state of well-developed Alfvénic turbulence, with low
  intermittency. This is interpreted in terms of slab turbulence in the
  context of nearly incompressible magnetohydrodynamics. Conversely,
  the highly intermittent and poorly developed turbulent behavior of the
  solar wind from the weaker magnetic field region is presumably due to
  large magnetic deflections most likely attributed to the presence of
  switchbacks of interchange reconnection origin.

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Title: Dark off-limb gap: manifestation of temperature minimum and
    dynamic nature of the chromosphere
Authors: Kuridze, D.; Heinzel, P.; Koza, J.; Oliver, R.
2022arXiv220814134K    Altcode:
  We study off-limb emission of the lower solar atmosphere using
  high-resolution imaging spectroscopy in the H$\beta$ and Ca II 8542 Å
  lines obtained with the CHROMospheric Imaging Spectrometer (CHROMIS)
  and the CRisp Imaging SpectroPolarimeter (CRISP) on the Swedish 1-m
  Solar Telescope. The H$\beta$ line wing images show the dark intensity
  gap between the photospheric limb and chromosphere which is absent
  in the Ca II images. We calculate synthetic spectra of the off-limb
  emissions with the RH code in the one-dimension spherical geometry and
  find good agreement with the observations. The analysis of synthetic
  line profiles shows that the gap in the H$\beta$ line wing images maps
  the temperature minimum region between the photosphere and chromosphere
  due to the well known opacity and emissivity gap of Balmer lines in this
  layer. However, observed gap is detected farther from the line core
  in the outer line wing positions than in the synthetic profiles. We
  found that an increased microturbulence in the model chromosphere is
  needed to reproduce the dark gap in the outer line wing, suggesting that
  observed H$\beta$ gap is the manifestation of the temperature minimum
  and the dynamic nature of the solar chromosphere. The temperature
  minimum produces a small enhancement in synthetic Ca II line-wing
  intensities. Observed off-limb Ca II line-wing emissions show similar
  enhancement below temperature minimum layer near the edge of the
  photospheric limb.

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Title: Data-driven Model of Temporal Evolution of Solar Mg II h and
    k Profiles over the Solar Cycle
Authors: Koza, Július; Gunár, Stanislav; Schwartz, Pavol; Heinzel,
   Petr; Liu, Wenjuan
2022ApJS..261...17K    Altcode:
  The solar radiation in the cores of the Mg II h and k spectral lines
  plays a significant role in the illumination of prominences, coronal
  mass ejections (CMEs), spicules, flare loops, and surges. Moreover,
  the radiation in these lines strongly correlates with solar magnetic
  activity and the ultraviolet solar spectral irradiance affecting
  the photochemistry, especially of oxygen and nitrogen, in the middle
  atmosphere of the Earth. This work provides a data-driven model of
  temporal evolution of the solar full-disk Mg II h and k profiles over
  the solar cycle. The capability of the model to reproduce the Mg II h
  and k profiles for an arbitrary date is statistically assessed. Based
  on selected 76 IRIS near-UV full-Sun mosaics covering almost the full
  solar cycle 24, we find the parameters of double-Gaussian fits of the
  disk-averaged Mg II h and k profiles and a model of their temporal
  evolution parameterized by the Bremen composite Mg II index. The
  model yields intensities within the uncertainties of the observed
  data in more than 90% of the reconstructed profiles assuming a
  statistically representative set of Bremen Mg II index values in the
  range of 0.150-0.165. The relevant full-disk Mg II h and k calibrated
  profiles with uncertainties and spectral irradiances are provided as an
  online machine-readable table. The model yields Mg II h and k profiles
  representing the disk incident radiation for the radiative-transfer
  modeling of prominences, CMEs, spicules, flare loops, and surges
  observed at arbitrary time.

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Title: Large Impact of the Mg II h and k Incident Radiation Change
    on Results of Radiative Transfer Models and the Importance of Dynamics
Authors: Gunár, Stanislav; Heinzel, Petr; Koza, Július; Schwartz,
   Pavol
2022ApJ...934..133G    Altcode:
  We demonstrate that changes in the incident radiation in Mg II h
  and k lines have a significant impact on the results of radiative
  transfer modeling of prominence-like plasmas. To uncover the extent
  of this impact and allow easy comparison, here we study two cases,
  one representing the minimum of the solar activity and the other
  corresponding to the typical conditions during solar maxima. To
  represent well the properties of the prominence plasma, we use the 2D
  non-LTE (i.e., departures from local thermodynamic equilibrium) model
  of prominence fine structures in both the single-thread configuration
  and the multithread configuration incorporating prominence dynamics. We
  show that in the modeled environment of prominence fine structures,
  the change in the central, integrated, and peak intensities of the
  synthetic Mg II h and k profiles can be as large as the change in the
  incident radiation itself. This means that the Mg II h and k spectra
  of observed prominences can be affected by tens of percent because the
  illumination from the solar disk can change by such a degree over the
  solar cycle. That makes the knowledge and use of event-specific incident
  radiation data very important for the diagnostics of prominences
  and other chromospheric and coronal structures when using Mg II h
  and k spectral observations. In addition, the observed Mg II h and k
  spectra are strongly influenced by the line-of-sight dynamics, as the
  multithread configuration of the 2D model allows us to reveal. The
  effect of dynamics is, unsurprisingly, most pronounced in the line
  widths and integrated intensities.

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Title: A first comparison of FLARIX flare simulations with the MSDP
    H-alpha spectral observations on very short time scales
Authors: Heinzel, Petr; Kasparova, Jana; Berlicki, Arkadiusz;
   Radziszewski, Krzysztof; Rudawy, Pawel
2022cosp...44.2560H    Altcode:
  We present first results of a comparative analysis of high temporal
  resolution MSDP H$\alpha$ observations of a compact solar flare with
  results of radiation-hydrodynamical simulations performed using the
  FLARIX code. X-ray spectral observations of a compact C1 GOES-class
  flare obtained from RHESSI satellite were used to estimate physical
  parameters of the electron beams transporting the energy from the
  reconnection site down to the chromosphere. These parameters are then
  used for data-driven FLARIX simulations. A small size of the flare
  and its simple structure allowed us to assume a single-loop geometry
  which significantly simplified the modelling and analysis of the
  whole event. Using the MSDP imaging spectrograph at Bia{\l}k\'{o}w
  observatory, it was possible to compare the recorded H$\alpha$
  line emission with that obtained from FLARIX simulations, on short
  time-scales down to 50 ms.

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Title: Geometry and dynamics of cool flare loops observed by IRIS
Authors: Mikuła, Katarzyna; Heinzel, Petr; Berlicki, Arkadiusz
2022cosp...44.2414M    Altcode:
  Flare loops represent a well-known, inseparable part of solar
  flares. They are observed mainly during the gradual phase of the flares,
  being rooted in flare ribbons. They can form an entire arcade which
  evolves in the corona, sometimes for hours. The loops are visible
  in a wide range of temperature bands, from X-rays (hot flare loops)
  to temperatures of the cool chromospheric-type plasma seen in the
  ultraviolet and optical spectrum (cool flare loops). We present
  results of our analysis of cool flare loops observed during the gradual
  phase of M6.5 solar flare on June 22, 2015 based on the ultraviolet
  observations obtained by Interface Region Imaging Spectrograph
  (IRIS). Detailed investigation of these loops, made on the basis of
  Mg II line profiles, was presented in Mikuła et al. (2017). Mg II
  line profiles were modelled using the standard cloud model method
  that allowed us obtaining simultaneously the physical parameters
  characteridsing the moving plasma inside selected loops, i.e. the
  velocity along the line-of-sight, microturbulent velocity, optical
  thickness, and the line source function. Here we present a next step
  of the work — reconstruction of the true shape of flare loops based
  on the geometric method of Loughhead, Wang and Blows (1983). Based
  on two-dimensional images of a given loop structure located on
  the solar disk or at the limb, we can obtain its true orientation
  and its size. The shape of the analysed loops was determined mainly
  from IRIS slit-jaw images at 1330, 1400 and 2796 \AA{}, supplemented
  with SDO/AIA 171 \AA{} images in some cases. Using basic geometry,
  we reconstructed the shape of selected loops in the three-dimensional
  space. Based on the method presented in Loughhead and Bray (1984) we
  were able to derive the so-called true velocity of the plasma flows,
  i.e. the velocity along the loop axis. The results obtained for each
  loop were then compared with the free fall velocities.

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Title: New Insight into UV Compact Bursts - Statistical Analysis of
    IRIS Data
Authors: Berlicki, Arkadiusz; Heinzel, Petr; Schmieder, Brigitte;
   Michalina Litwicka, M.
2022cosp...44.2532B    Altcode:
  UV small-scale brightenings have been frequently observed by IRIS in
  both NUV and FUV channels. They appear as compact and intense, but short
  lived bursts visible within the solar active regions. Some of them seem
  to be closely connected with the well-known Ellerman bombs and so-called
  IRIS bombs. Based on the IRIS observations of many compact bursts
  obtained in chromospheric Mg II h and k lines, Mg II triplet and FUV
  lines we present detailed statistical analysis of these phenomena. In
  the work of Grubecka et al. (2016), five different compact bursts (CBs)
  were selected and analysed in detail. NLTE semi-empirical models of
  them were constructed based on their spectral characteristics in the
  Mg II h and k lines. In addition, they were preliminarily categorised
  into three types. In present work we extend previous analysis and
  investigate statistical diversity of Mg II lines of UV bursts and
  their visibility in FUV lines such as Si IV or C II. IRIS database
  from 2013-2018 was searched for dense rasters of active and emerging
  flux regions containing spectra in Mg II, C II and Si IV. A next step
  was to reconstruct full rasters in which we were looking for compact
  brightenings with size of the order of one arcsec. We found more than
  two thousands CBs using criteria based on specific parameters of the
  Mg II k line profile. In addition, we analysed also the emission of
  Mg II UV triplet and some parameters of Si IV and C II lines. This
  database allowed us to make a novel statistical analysis of all bursts
  and we categorised them in previously defined three types, depending on
  their Mg II line profiles shapes. We also investigated the correlations
  between the emission of Mg II lines, "hotter" Si IV lines, and C II
  lines in order to find which of these events are linked with IRIS bombs
  (Peter et al. 2014). Finally, we analysed some observables of those
  UV bursts, which can be defined as candidates for Ellerman bombs.

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Title: Diagnostics of The Prominence Plasma Based on IRIS, H-alpha
    and ALMA Observations
Authors: Berlicki, Arkadiusz; Bárta, Miroslav; Gunár, Stanislav;
   Heinzel, Petr; Jejcic, Sonja; Radziszewski, Krzysztof; Rudawy, Pawel
2022cosp...44.2543B    Altcode:
  Solar prominences are now commonly observed above the solar limb in
  different spectral bands and recent developments of new observing
  techniques allow us to detect them from radio to far-UV ranges. In
  addition to often used spectral observations in optical and UV,
  ALMA interferometer obtained high-resolution images of a quiescent
  solar prominence at 3 millimeters (Band 3) during the coordinated
  space and ground-based observing campaign. For the first time
  high-resolution observations of such structures in the millimeter
  radio domain are available. The fine structures of this prominence was
  also observed in the UV with IRIS and in the H$\alpha$ line with the
  MSDP of Wroc{\l}aw Observatory. Both UV and H$\alpha$ data contains
  not only images, but also spectra which makes the available dataset
  extremely valuable. Moreover, all UV, H$\alpha$ and ALMA observations
  are co-temporal which gives an unprecedented opportunity for a novel
  diagnostic, not available so far. In this work we present analysis
  of the prominence spectral characteristics in H$\alpha$ and UV Mg
  II lines, looking for the statistical dependence between different
  parameters (metrics) in the line profiles. This combined data is
  then used for determination of plasma parameters in the prominence
  fine structures. In addition, UV and H$\alpha$ spectral maps are
  compared with the brightness temperature mosaics from ALMA, providing
  an additional constraint on the plasma kinetic temperature. Detailed
  diagnostics is then based on extensive NLTE numerical simulations of
  the radiative transfer inside heterogeneous prominence structures.

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Title: Spectral line asymmetries observed during stellar flares
Authors: Wollmann, Jiří; Heinzel, Petr; Kabath, Petr; Karjalainen,
   Raine; Skarka, Marek; Špoková, Magdalena
2022cosp...44.2468W    Altcode:
  Stellar flares are highly energetic events occuring in stellar
  atmospheres. This solar-like activity has been observed on G, K and M
  stars. Red dwarfs usually have vast and strong magnetic fields which
  often reconnect and produce strong flares, sometimes classified as the
  so-called superflares. From spectroscopic observations we see, apart
  from typical enhancements of the line intensities, clearly asymmetrical
  line profiles. In analogy with solar flares, one would interpret them
  as due to flows in the flaring chromosphere. However, some stellar
  observations indicate a peculiar behaviour of such asymmetries and
  their nature is not well understood. In this work we present recent
  spectroscopic observations of flares on AD Leo star obtained with the
  Ondrejov Echelle Spectrograph. We analyze detected asymmetries using
  the non-LTE radiative-transfer modeling and demonstrate the importance
  of flare dynamics. Our interpretation is based on a close analogy with
  solar flares.

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Title: Mini solar flare and jet due to small scale surface motions
Authors: Joshi, Reetika; Vilmer, Nicole; Chandra, Ramesh; Heinzel,
   Petr; Bommier, Veronique; Schmieder, Brigitte; Aulanier, Guillaume;
   Tomin, James
2022cosp...44.2535J    Altcode:
  Here we present the study of the fine structure and dynamics of the
  plasma at a jet base forming a mini-flare between two emerging magnetic
  fluxes (EMFs) observed with Interface Region Imaging Spectrograph
  (IRIS) and the Solar Dynamics Observatory instruments. This active
  region is an outcome of the collapse of two EMFs overlaid by arch
  filament systems. We observed that, before the jet an extension of
  the flux rope was present and a part of it was detached and formed
  a small bipole with a bald patch region, which dynamically became
  an X-current sheet over the dome of one EMF where the reconnection
  took place. At the time in the site of reconnection, the IRIS C II,
  Si IV, and Mg II line profiles present bi directional flows in a tiny
  region. These types of spectra are typically associated with twist,
  rotation, or the presence of plasma in helical structures. The tilt
  observed in our spectra can be explained by the presence of a helical
  structure at the jet base during the reconnection process due to a
  transfer of the twist from a flux rope in the vicinity of the jet. We
  also combined the observations of the Balmer continuum obtained with
  the IRIS (spectra and SJIs 2832 Å). The calibrated Balmer continuum
  was compared to non-local thermodynamic equilibrium radiative transfer
  flare models and the radiated energy was estimated. Assuming thick
  target HXR emission, we calculated the energy of the non thermal
  electrons detected by the Fermi/GBM and compared it to the radiated
  energy. The electron-beam flux estimated from Fermi/GBM between 10$
  ^{9}$ and 10$ ^{10}$ erg s$ ^{-1}$ cm$ ^{-2}$ is consistent with the
  beam flux required in non-LTE radiative transfer models to obtain the
  excess of Balmer continuum emission observed in this IRIS spectra. We
  conclude that the bombardment of electrons could be in a region smaller
  than the IRIS spatial resolution.

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Title: Variability of solar Lyman-alpha and Mg II h&amp;k lines
    throughout the solar cycle and its impact on the diagnostics of
    chromospheric and coronal structures
Authors: Gunár, Stanislav; Schwartz, Pavol; Heinzel, Petr; Liu,
   Wenjuan; Koza, Julius
2022cosp...44.1553G    Altcode:
  The solar radiation in the Lyman-alpha and Mg II h&amp;k spectral lines
  plays a crucial role in the illumination of chromospheric and coronal
  structures, such as prominences/filaments, spicules, chromospheric
  fibrils, cores of coronal mass ejections, or solar wind. Moreover,
  it is important for the investigation of the heliosphere, Earth
  ionosphere, and the atmospheres of planets, moons, and comets. However,
  the emissivity of the Sun is not constant in these lines but changes
  considerably throughout the solar cycle. To study these changes
  and their impact, we first had to set the baseline representing the
  radiation from the solar disk during a minimum of solar activity. We
  thus derived new sets of quiet-Sun reference profiles of Lyman-alpha
  and Mg II h&amp;k lines. For the Lyman-alpha line, we used SOHO/SUMER
  raster scans obtained without the use of the SUMER attenuator (Gunár et
  al. 2020) and for the Mg II h&amp;k lines we used the broad catalogue of
  IRIS full-Sun mosaics (Gunár et al. 2021). To quantify the variability
  with the solar cycle, we used the LISIRD Composite Lyman-alpha index to
  adapt the Lyman lines to any specific date (Gunár et al. 2020). For
  the Mg II h&amp;k lines, we used a data-driven model based on the
  Bremen Composite Mg II index (Koza et al. 2022). These long-term
  measures then allowed us to investigate how the changing irradiation
  from the solar surface influences the synthetic spectra produced by
  the radiative transfer modelling. As we showed in Gunár et al. (2020,
  2022), both changes in the Lyman lines and the Mg II h&amp;k lines
  affect the resulting synthetic spectra significantly, even up to 50 %
  depending on the strength of individual solar cycles. That, however,
  has a strong impact on the diagnostics of the observed chromospheric
  and coronal structures, making up-to-date information about the solar
  activity a critical input for their precise modelling.

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Title: Doppler-velocity Drifts Detected in a Solar Prominence
Authors: Zapiór, Maciej; Heinzel, Petr; Khomenko, Elena
2022ApJ...934...16Z    Altcode:
  We analyzed multiline observations of a quiescent prominence from the
  slit spectrograph located at the Ondřejov Observatory. Dopplergrams
  and integrated intensity maps of the whole prominence were obtained
  from observations in six spectral lines: Ca II H, Hϵ, Hβ, He I D3,
  Hα, and Ca II IR. By combining integrated intensity maps with non-LTE
  radiative-transfer modeling, we carefully identified areas in an
  optically thin regime. The comparison of the Doppler-velocity maps and
  scatterplots from different lines shows the existence of differences
  in the velocity of ions and neutrals called velocity drift. The drift
  is of a local nature, present mostly at prominence edges in the area
  with a large velocity gradient, as can be tentatively expected based on
  multifluid MHD models. We could not explore the time evolution of the
  drift, since our data set consists of a single scan only. Our paper
  brings another contribution to a rather controversial problem of the
  detection of multifluid effects in solar prominences.

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Title: Modeling Balmer line signatures of stellar CMEs
Authors: Leitzinger, M.; Odert, P.; Heinzel, P.
2022MNRAS.513.6058L    Altcode: 2022MNRAS.tmp.1287L; 2022arXiv220503110L
  From the Sun, we know that coronal mass ejections (CMEs) are a
  transient phenomenon, often correlated with flares. They have an
  impact on solar mass- and angular momentum loss, and therefore solar
  evolution, and make a significant part of space weather. The same
  is true for stars, but stellar CMEs are still not well constrained,
  although new methodologies have been established, and new detections
  presented in the recent past. So far, probable detections of stellar
  CMEs have been presented, but their physical parameters which are
  not directly accessible from observations, such as electron density,
  optical thickness, temperature, etc., have been so far not determined
  for the majority of known events. We apply cloud modeling, as commonly
  used on the Sun, to a known event from the literature, detected on
  the young dMe star V374 Peg. This event manifests itself in extra
  emission on the blue side of the Balmer lines. By determining the line
  source function from 1D NLTE modeling together with the cloud model
  formulation, we present distributions of physical parameters of this
  event. We find that except for temperature and area all parameters
  are at the upper range of typical solar prominence parameters. The
  temperature and the area of the event were found to be higher than
  for typical solar prominences observed in Balmer lines. We find more
  solutions for the filament than for the prominence geometry. Moreover,
  we show that filaments can appear in emission on dMe stars contrary
  to the solar case.

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Title: Prominence eruption observed in He II 304 Å up to &gt;6
    R<SUB>⊙</SUB> by EUI/FSI aboard Solar Orbiter
Authors: Mierla, M.; Zhukov, A. N.; Berghmans, D.; Parenti, S.;
   Auchère, F.; Heinzel, P.; Seaton, D. B.; Palmerio, E.; Jejčič, S.;
   Janssens, J.; Kraaikamp, E.; Nicula, B.; Long, D. M.; Hayes, L. A.;
   Jebaraj, I. C.; Talpeanu, D. -C.; D'Huys, E.; Dolla, L.; Gissot, S.;
   Magdalenić, J.; Rodriguez, L.; Shestov, S.; Stegen, K.; Verbeeck,
   C.; Sasso, C.; Romoli, M.; Andretta, V.
2022A&A...662L...5M    Altcode: 2022arXiv220515214M
  <BR /> Aims: We report observations of a unique, large prominence
  eruption that was observed in the He II 304 Å passband of the Extreme
  Ultraviolet Imager/Full Sun Imager telescope aboard Solar Orbiter on
  15-16 February 2022. <BR /> Methods: Observations from several vantage
  points - Solar Orbiter, the Solar-Terrestrial Relations Observatory,
  the Solar and Heliospheric Observatory, and Earth-orbiting satellites -
  were used to measure the kinematics of the erupting prominence and the
  associated coronal mass ejection. Three-dimensional reconstruction was
  used to calculate the deprojected positions and speeds of different
  parts of the prominence. Observations in several passbands allowed us
  to analyse the radiative properties of the erupting prominence. <BR />
  Results: The leading parts of the erupting prominence and the leading
  edge of the corresponding coronal mass ejection propagate at speeds
  of around 1700 km s<SUP>−1</SUP> and 2200 km s<SUP>−1</SUP>,
  respectively, while the trailing parts of the prominence are
  significantly slower (around 500 km s<SUP>−1</SUP>). Parts of the
  prominence are tracked up to heights of over 6 R<SUB>⊙</SUB>. The
  He II emission is probably produced via collisional excitation rather
  than scattering. Surprisingly, the brightness of a trailing feature
  increases with height. <BR /> Conclusions: The reported prominence
  is the first observed in He II 304 Å emission at such a great
  height (above 6 R<SUB>⊙</SUB>). <P />Movies are available at <A
  href="https://www.aanda.org/10.1051/0004-6361/202244020/olm">https://www.aanda.org</A>

---------------------------------------------------------
Title: Observation of Magnetic Switchback in the Solar Corona
Authors: Telloni, Daniele; Zank, Gary P.; Stangalini, Marco;
   Downs, Cooper; Liang, Haoming; Nakanotani, Masaru; Andretta,
   Vincenzo; Antonucci, Ester; Sorriso-Valvo, Luca; Adhikari, Laxman;
   Zhao, Lingling; Marino, Raffaele; Susino, Roberto; Grimani, Catia;
   Fabi, Michele; D'Amicis, Raffaella; Perrone, Denise; Bruno, Roberto;
   Carbone, Francesco; Mancuso, Salvatore; Romoli, Marco; Da Deppo, Vania;
   Fineschi, Silvano; Heinzel, Petr; Moses, John D.; Naletto, Giampiero;
   Nicolini, Gianalfredo; Spadaro, Daniele; Teriaca, Luca; Frassati,
   Federica; Jerse, Giovanna; Landini, Federico; Pancrazzi, Maurizio;
   Russano, Giuliana; Sasso, Clementina; Berghmans, David; Auchère,
   Frédéric; Aznar Cuadrado, Regina; Chitta, Lakshmi P.; Harra, Louise;
   Kraaikamp, Emil; Long, David M.; Mandal, Sudip; Parenti, Susanna;
   Pelouze, Gabriel; Peter, Hardi; Rodriguez, Luciano; Schühle, Udo;
   Schwanitz, Conrad; Smith, Phil J.; Verbeeck, Cis; Zhukov, Andrei N.
2022arXiv220603090T    Altcode:
  Switchbacks are sudden, large radial deflections of the solar wind
  magnetic field, widely revealed in interplanetary space by the Parker
  Solar Probe. The switchbacks' formation mechanism and sources are still
  unresolved, although candidate mechanisms include Alfvénic turbulence,
  shear-driven Kelvin-Helmholtz instabilities, interchange reconnection,
  and geometrical effects related to the Parker spiral. This Letter
  presents observations from the Metis coronagraph onboard Solar Orbiter
  of a single large propagating S-shaped vortex, interpreted as first
  evidence of a switchback in the solar corona. It originated above
  an active region with the related loop system bounded by open-field
  regions to the East and West. Observations, modeling, and theory provide
  strong arguments in favor of the interchange reconnection origin of
  switchbacks. Metis measurements suggest that the initiation of the
  switchback may also be an indicator of the origin of slow solar wind.

---------------------------------------------------------
Title: Non-LTE Inversion of Prominence Spectroscopic Observations
    in Hα and Mg II h&amp;k lines
Authors: Jejčič, Sonja; Heinzel, Petr; Schmieder, Brigitte; Gunár,
   Stanislav; Mein, Pierre; Mein, Nicole; Ruan, Guiping
2022ApJ...932....3J    Altcode:
  We continued our investigation of the plasma characteristics of a
  quiescent prominence that occurred on 2017 March 30. The prominence
  was observed simultaneously by several instruments, including the
  Interface Region Imaging Spectrograph (IRIS) and the Multichannel
  Subtractive Double Pass (MSDP) spectrograph operating at the Meudon
  solar tower. We focused on IRIS Mg II h&amp;k and MSDP Hα spectra,
  selecting 55 well-coaligned points within the prominence. We computed
  an extensive grid of 63,000 isothermal and isobaric 1D-slab prominence
  models with a non-LTE (i.e., departures from the local thermodynamic
  equilibrium) radiative transfer code. We then performed a 1.5D
  spectral inversion searching for an optimal model that best fits
  five parameters of the observed profiles (observables), namely,
  the integrated intensity of the Hα and Mg II k lines, the FWHM of
  both lines, and the ratio of intensities of the Mg II k and Mg II h
  lines. The latter is sensitive to temperature. Our results show that
  the prominence is a low-temperature structure, mostly below 10,000
  K, with some excursions to higher values (up to 18,000 K) but also
  rather low temperatures (around 5000 K). The microturbulent velocity is
  typically low, peaking around 8 km s<SUP>-1</SUP>, and electron density
  values are of the order of 10<SUP>10</SUP> cm<SUP>-3</SUP>. The peak
  effective thickness is 500 km, although the values range up to 5000
  km. The studied prominence is rather optically thin in the Hα line
  and optically thick in the Mg II h&amp;k lines.

---------------------------------------------------------
Title: Subarcsecond Imaging of a Solar Active Region Filament With
    ALMA and IRIS
Authors: da Silva Santos, J. M.; White, S. M.; Reardon, K.; Cauzzi,
   G.; Gunár, S.; Heinzel, P.; Leenaarts, J.
2022FrASS...9.8115D    Altcode: 2022arXiv220413178D
  Quiescent filaments appear as absorption features on the solar disk
  when observed in chromospheric lines and at continuum wavelengths
  in the millimeter (mm) range. Active region (AR) filaments are their
  small-scale, low-altitude analogues, but they could not be resolved
  in previous mm observations. This spectral diagnostic can provide
  insight into the details of the formation and physical properties of
  their fine threads, which are still not fully understood. Here, we shed
  light on the thermal structure of an AR filament using high-resolution
  brightness temperature (Tb) maps taken with ALMA Band 6 complemented by
  simultaneous IRIS near-UV spectra, Hinode/SOT photospheric magnetograms,
  and SDO/AIA extreme-UV images. Some of the dark threads visible in the
  AIA 304 Å passband and in the core of Mg ii resonance lines have dark
  (Tb &lt; 5,000 K) counterparts in the 1.25 mm maps, but their visibility
  significantly varies across the filament spine and in time. These
  opacity changes are possibly related to variations in temperature and
  electron density in filament fine structures. The coolest Tb values
  (&lt; 5,000 K) coincide with regions of low integrated intensity in the
  Mg ii h and k lines. ALMA Band 3 maps taken after the Band 6 ones do not
  clearly show the filament structure, contrary to the expectation that
  the contrast should increase at longer wavelengths based on previous
  observations of quiescent filaments. The ALMA maps are not consistent
  with isothermal conditions, but the temporal evolution of the filament
  may partly account for this.

---------------------------------------------------------
Title: ALMA as a Prominence Thermometer: First Observations
Authors: Heinzel, Petr; Berlicki, Arkadiusz; Bárta, Miroslav; Rudawy,
   Paweł; Gunár, Stanislav; Labrosse, Nicolas; Radziszewski, Krzysztof
2022ApJ...927L..29H    Altcode: 2022arXiv220212761H
  We present first prominence observations obtained with Atacama
  Large Millimeter Array (ALMA) in Band 3 at the wavelength of
  3 mm. High-resolution observations have been coaligned with the
  MSDP Hα data from Wrocław-Białków large coronagraph at similar
  spatial resolution. We analyze one particular cotemporal snapshot,
  first calibrating both ALMA and MSDP data and then demonstrating a
  reasonable correlation between both. In particular, we can see quite
  similar fine-structure patterns in both ALMA brightness-temperature maps
  and MSDP maps of Hα intensities. Using ALMA, we intend to derive the
  prominence kinetic temperatures. However, having current observations
  only in one band, we use an independent diagnostic constraint, which
  is the Hα line integrated intensity. We develop an inversion code and
  show that it can provide realistic temperatures for brighter parts of
  the prominence where one gets a unique solution, while within faint
  structures, such inversion is ill conditioned. In brighter parts,
  ALMA serves as a prominence thermometer, provided that the optical
  thickness in Band 3 is large enough. In order to find a relation between
  brightness and kinetic temperatures for a given observed Hα intensity,
  we constructed an extended grid of non-LTE prominence models covering
  a broad range of prominence parameters. We also show the effect of
  the plane-of-sky filling factor on our results.

---------------------------------------------------------
Title: Constraining stellar CMEs by solar observations
Authors: Leitzinger, Martin; Odert, Petra; Leka, K. D.; Heinzel,
   Petr; Dissauer, Karin
2021AGUFM.U43B..06L    Altcode:
  Stellar coronal mass ejections (CMEs) may play an important role
  in star-planet interactions, such as planetary atmospheric escape,
  and in stellar mass- and angular momentum loss, influencing stellar
  evolution. In the last decades much effort has been put into determining
  parameters of stellar CMEs. New detection methods have been developed,
  but still the number of convincing events is low and far from
  enabling statistical analyses. So far the methods of detections
  comprise the direct signature of ejected plasma, namely Doppler
  shifted emission/absorption visible in spectra (optical, UV, X-ray),
  absorptions seen during flares in X-rays interpreted as obscuring
  events, and CME-associated signatures known from the Sun, like radio
  type II bursts and coronal dimmings, the latter being only recently
  established. The first method (Doppler shifted emission/absorption
  lines) has been used since decades on stars (especially in H which
  well probes the eruptive filament/prominence in the CME core) and
  provides a few convincing detections and a large number of candidate
  events with projected velocities significantly below the stars' escape
  velocities. Such events could be CMEs seen in projection but it has
  been proposed that these signatures could be caused by flare related
  plasma dynamics. As there is a large pool of candidate events which
  cannot be unambiguously interpreted as CMEs, we propose a new approach
  to distinguish between flare and CME related signtures to increase the
  number of convincing CME events. What we observe from stars are disk
  integrated signals, in contrast to solar observations. To constrain
  stellar CMEs by solar observations, solar 2D imaging spectroscopy is
  required from which spatially integrated spectra can be created for a
  sufficiently large number of events (flares and CMEs). These aspects
  are fulfilled by MEES CCD (MCCD) optical observations at Mees Solar
  Observatory (MSO). Therefore we propose the analysis of a sample of
  solar flares and filaments/prominences from MCCD/MSO and their spatially
  integrated spectra which allows to separate contributions from flares
  and filaments/prominences. We present preliminary results of a few
  selected solar events from MCCD demonstrating how to characterize
  flare and CME related signatures in stellar observations.

---------------------------------------------------------
Title: Empirical atmosphere model in a mini flare during magnetic
    reconnection
Authors: Schmieder, Brigitte; Joshi, Reetika; Chandra, Ramesh;
   Aulanier, Guillaume; Tei, Akiko; Heinzel, Petr; Tomin, James; Vilmer,
   Nicole; Bommier, Veronique
2021arXiv211206790S    Altcode:
  A spatio-temporal analysis of IRIS spectra of MgII, CII, and SiIV ions
  allows us to study the dynamics and the stratification of the flare
  atmosphere along the line of sight during the magnetic reconnection
  phase at the jet base. Strong asymmetric MgII and CII line profiles with
  extended blue wings observed at the reconnection site are interpreted
  by the presence of two chromospheric temperature clouds: one explosive
  cloud with blueshifts at 290 km/s and one cloud with smaller Doppler
  shift (around 36 km/s). Simultaneously at the same location a mini
  flare was observed with strong emission in multi temperatures (AIA),
  in several spectral IRIS lines (e.g. Oiv and Siiv, Mgii), absorption
  of identified chromospheric lines in Siiv line profile, enhancement
  of the Balmer continuum and X-ray emission by FERMI/GBM. With the
  standard thick-target flare model we calculate the energy of non thermal
  electrons observed by FERMI and compare it to the energy radiated by
  the Balmer continuum emission. We show that the low energy input by
  non thermal electrons above 20 keV was still sufficient to produce
  the excess of Balmer continuum.

---------------------------------------------------------
Title: The first coronal mass ejection observed in both visible-light
    and UV H I Ly-α channels of the Metis coronagraph on board Solar
    Orbiter
Authors: Andretta, V.; Bemporad, A.; De Leo, Y.; Jerse, G.; Landini,
   F.; Mierla, M.; Naletto, G.; Romoli, M.; Sasso, C.; Slemer, A.;
   Spadaro, D.; Susino, R.; Talpeanu, D. -C.; Telloni, D.; Teriaca, L.;
   Uslenghi, M.; Antonucci, E.; Auchère, F.; Berghmans, D.; Berlicki,
   A.; Capobianco, G.; Capuano, G. E.; Casini, C.; Casti, M.; Chioetto,
   P.; Da Deppo, V.; Fabi, M.; Fineschi, S.; Frassati, F.; Frassetto,
   F.; Giordano, S.; Grimani, C.; Heinzel, P.; Liberatore, A.; Magli, E.;
   Massone, G.; Messerotti, M.; Moses, D.; Nicolini, G.; Pancrazzi, M.;
   Pelizzo, M. -G.; Romano, P.; Schühle, U.; Stangalini, M.; Straus,
   Th.; Volpicelli, C. A.; Zangrilli, L.; Zuppella, P.; Abbo, L.; Aznar
   Cuadrado, R.; Bruno, R.; Ciaravella, A.; D'Amicis, R.; Lamy, P.;
   Lanzafame, A.; Malvezzi, A. M.; Nicolosi, P.; Nisticò, G.; Peter,
   H.; Plainaki, C.; Poletto, L.; Reale, F.; Solanki, S. K.; Strachan,
   L.; Tondello, G.; Tsinganos, K.; Velli, M.; Ventura, R.; Vial, J. -C.;
   Woch, J.; Zimbardo, G.
2021A&A...656L..14A    Altcode:
  Context. The Metis coronagraph on board Solar Orbiter offers a new
  view of coronal mass ejections (CMEs), observing them for the first
  time with simultaneous images acquired with a broad-band filter in
  the visible-light interval and with a narrow-band filter around the
  H I Ly-α line at 121.567 nm, the so-called Metis UV channel. <BR />
  Aims: We show the first Metis observations of a CME, obtained on 16
  and 17 January 2021. The event was also observed by the EUI/FSI imager
  on board Solar Orbiter, as well as by other space-based coronagraphs,
  such as STEREO-A/COR2 and SOHO/LASCO/C2, whose images are combined here
  with Metis data. <BR /> Methods: Different images are analysed here
  to reconstruct the 3D orientation of the expanding CME flux rope using
  the graduated cylindrical shell model. This also allows us to identify
  the possible location of the source region. Measurements of the CME
  kinematics allow us to quantify the expected Doppler dimming in the
  Ly-α channel. <BR /> Results: Observations show that most CME features
  seen in the visible-light images are also seen in the Ly-α images,
  although some features in the latter channel appear more structured
  than their visible-light counterparts. We estimated the expansion
  velocity of this event to be below 140 km s<SUP>−1</SUP>. Hence,
  these observations can be understood by assuming that Doppler dimming
  effects do not strongly reduce the Ly-α emission from the CME. These
  velocities are comparable with or smaller than the radial velocities
  inferred from the same data in a similar coronal structure on the
  east side of the Sun. <BR /> Conclusions: The first observations by
  Metis of a CME demonstrate the capability of the instrument to provide
  valuable and novel information on the structure and dynamics of these
  coronal events. Considering also its diagnostics capabilities regarding
  the conditions of the ambient corona, Metis promises to significantly
  advance our knowledge of such phenomena. <P />Movies are available at <A
  href="https://www.aanda.org/10.1051/0004-6361/202142407/olm">https://www.aanda.org</A>

---------------------------------------------------------
Title: Cosmic-ray flux predictions and observations for and with
    Metis on board Solar Orbiter
Authors: Grimani, C.; Andretta, V.; Chioetto, P.; Da Deppo, V.; Fabi,
   M.; Gissot, S.; Naletto, G.; Persici, A.; Plainaki, C.; Romoli, M.;
   Sabbatini, F.; Spadaro, D.; Stangalini, M.; Telloni, D.; Uslenghi, M.;
   Antonucci, E.; Bemporad, A.; Capobianco, G.; Capuano, G.; Casti, M.;
   De Leo, Y.; Fineschi, S.; Frassati, F.; Frassetto, F.; Heinzel, P.;
   Jerse, G.; Landini, F.; Liberatore, A.; Magli, E.; Messerotti, M.;
   Moses, D.; Nicolini, G.; Pancrazzi, M.; Pelizzo, M. G.; Romano, P.;
   Sasso, C.; Schühle, U.; Slemer, A.; Straus, T.; Susino, R.; Teriaca,
   L.; Volpicelli, C. A.; Freiherr von Forstner, J. L.; Zuppella, P.
2021A&A...656A..15G    Altcode: 2021arXiv210413700G
  Context. The Metis coronagraph is one of the remote sensing instruments
  hosted on board the ESA/NASA Solar Orbiter mission. Metis is devoted
  to carry out the first simultaneous imaging of the solar corona in
  both visible light (VL) and ultraviolet (UV). High-energy particles
  can penetrate spacecraft materials and may limit the performance of
  the on-board instruments. A study of the galactic cosmic-ray (GCR)
  tracks observed in the first VL images gathered by Metis during the
  commissioning phase is presented here. A similar analysis is planned
  for the UV channel. <BR /> Aims: We aim to formulate a prediction of
  the GCR flux up to hundreds of GeV for the first part of the Solar
  Orbiter mission to study the performance of the Metis coronagraph. <BR
  /> Methods: The GCR model predictions are compared to observations
  gathered on board Solar Orbiter by the High-Energy Telescope in the
  range between 10 MeV and 100 MeV in the summer of 2020 as well as with
  the previous measurements. Estimated cosmic-ray fluxes above 70 MeV
  n<SUP>−1</SUP> have been also parameterized and used for Monte Carlo
  simulations aimed at reproducing the cosmic-ray track observations in
  the Metis coronagraph VL images. The same parameterizations can also
  be used to study the performance of other detectors. <BR /> Results:
  By comparing observations of cosmic-ray tracks in the Metis VL images
  with FLUKA Monte Carlo simulations of cosmic-ray interactions in
  the VL detector, we find that cosmic rays fire only a fraction, on
  the order of 10<SUP>−4</SUP>, of the whole image pixel sample. We
  also find that the overall efficiency for cosmic-ray identification
  in the Metis VL images is approximately equal to the contribution
  of Z ≥ 2 GCR particles. A similar study will be carried out during
  the whole of the Solar Orbiter's mission duration for the purposes of
  instrument diagnostics and to verify whether the Metis data and Monte
  Carlo simulations would allow for a long-term monitoring of the GCR
  proton flux.

---------------------------------------------------------
Title: First light observations of the solar wind in the outer corona
    with the Metis coronagraph
Authors: Romoli, M.; Antonucci, E.; Andretta, V.; Capuano, G. E.; Da
   Deppo, V.; De Leo, Y.; Downs, C.; Fineschi, S.; Heinzel, P.; Landini,
   F.; Liberatore, A.; Naletto, G.; Nicolini, G.; Pancrazzi, M.; Sasso,
   C.; Spadaro, D.; Susino, R.; Telloni, D.; Teriaca, L.; Uslenghi,
   M.; Wang, Y. -M.; Bemporad, A.; Capobianco, G.; Casti, M.; Fabi, M.;
   Frassati, F.; Frassetto, F.; Giordano, S.; Grimani, C.; Jerse, G.;
   Magli, E.; Massone, G.; Messerotti, M.; Moses, D.; Pelizzo, M. -G.;
   Romano, P.; Schühle, U.; Slemer, A.; Stangalini, M.; Straus, T.;
   Volpicelli, C. A.; Zangrilli, L.; Zuppella, P.; Abbo, L.; Auchère,
   F.; Aznar Cuadrado, R.; Berlicki, A.; Bruno, R.; Ciaravella, A.;
   D'Amicis, R.; Lamy, P.; Lanzafame, A.; Malvezzi, A. M.; Nicolosi,
   P.; Nisticò, G.; Peter, H.; Plainaki, C.; Poletto, L.; Reale, F.;
   Solanki, S. K.; Strachan, L.; Tondello, G.; Tsinganos, K.; Velli,
   M.; Ventura, R.; Vial, J. -C.; Woch, J.; Zimbardo, G.
2021A&A...656A..32R    Altcode: 2021arXiv210613344R
  In this work, we present an investigation of the wind in the solar
  corona that has been initiated by observations of the resonantly
  scattered ultraviolet emission of the coronal plasma obtained with
  UVCS-SOHO, designed to measure the wind outflow speed by applying
  Doppler dimming diagnostics. Metis on Solar Orbiter complements the
  UVCS spectroscopic observations that were performed during solar
  activity cycle 23 by simultaneously imaging the polarized visible
  light and the H I Lyman-α corona in order to obtain high spatial and
  temporal resolution maps of the outward velocity of the continuously
  expanding solar atmosphere. The Metis observations, taken on May 15,
  2020, provide the first H I Lyman-α images of the extended corona
  and the first instantaneous map of the speed of the coronal plasma
  outflows during the minimum of solar activity and allow us to identify
  the layer where the slow wind flow is observed. The polarized visible
  light (580-640 nm) and the ultraviolet H I Lyα (121.6 nm) coronal
  emissions, obtained with the two Metis channels, were combined in
  order to measure the dimming of the UV emission relative to a static
  corona. This effect is caused by the outward motion of the coronal
  plasma along the direction of incidence of the chromospheric photons
  on the coronal neutral hydrogen. The plasma outflow velocity was then
  derived as a function of the measured Doppler dimming. The static
  corona UV emission was simulated on the basis of the plasma electron
  density inferred from the polarized visible light. This study leads
  to the identification, in the velocity maps of the solar corona, of
  the high-density layer about ±10° wide, centered on the extension
  of a quiet equatorial streamer present at the east limb - the coronal
  origin of the heliospheric current sheet - where the slowest wind
  flows at about 160 ± 18 km s<SUP>−1</SUP> from 4 R<SUB>⊙</SUB>
  to 6 R<SUB>⊙</SUB>. Beyond the boundaries of the high-density layer,
  the wind velocity rapidly increases, marking the transition between
  slow and fast wind in the corona.

---------------------------------------------------------
Title: Analysis and modeling of the dynamics of the glow of calcium
    and hydrogen lines in solar and stellar flares
Authors: Kupryakov, Yurij Alekseevich; Bychkov, Konstantin
   Veniaminovich; Belova, Oksana Mikhailovna; Gorshkov, Alexey Borisovich;
   Heinzel, Petr; Kotrč, Pavel
2021OAst...30...91K    Altcode:
  We present intensity curves of solar flares obtained in the Hα hydrogen
  line and CaII H, CaIR 8542Å lines using multichannel spectrographs of
  Ondřejov Observatory (Czech Republic) for the period 2000-2012. The
  general behavior of observed intensity curves is practically the same
  for all flares and is consistent with temporal variations of X-ray
  emission. However, our results differ significantly from those obtained
  by other authors for selected flare stars, for example, AD Leo; EV Lac;
  YZ CMi. We tried to explain the difference in the behavior of Ca II
  and Hα radiation flux by appearance of a shock wave during a flare
  and slow heating of the plasma.

---------------------------------------------------------
Title: Balmer continuum enhancement detected in a mini flare observed
    with IRIS
Authors: Joshi, Reetika; Schmieder, Brigitte; Heinzel, Petr; Tomin,
   James; Chandra, Ramesh; Vilmer, Nicole
2021A&A...654A..31J    Altcode: 2021arXiv210711651J
  Context. Optical and near-UV continuum emissions in flares contribute
  substantially to the flare energy budget. Two mechanisms play an
  important role for continuum emission in flares: hydrogen recombination
  after sudden ionization at chromospheric layers, and transportation of
  the energy radiatively from the chromosphere to lower layers in the
  atmosphere, the so-called back-warming. <BR /> Aims: The aim of the
  paper is to distinguish between these two mechanisms for the excess of
  the Balmer continuum observed in a flare. <BR /> Methods: We combined
  the observations of the Balmer continuum obtained with the Interface
  Region Imaging Spectrograph (IRIS) (spectra and slit-jaw images (SJIs)
  2832 Å) and hard X-ray (HXR) emission detected by the Fermi/Gamma Burst
  Monitor (GBM) during a mini flare. The calibrated Balmer continuum
  was compared to non-local thermodynamic equilibrium (LTE) radiative
  transfer flare models, and the radiated energy was estimated. Assuming
  thick target HXR emission, we calculated the energy of the nonthermal
  electrons detected by the Fermi/GBM and compared it to the radiated
  energy. <BR /> Results: The favorable argument of a relation between
  the Balmer continuum excess and the HXR emission is that there is
  a good time coincidence between them. In addition, the shape of the
  maximum brightness in the 2832 SJIs, which is mainly due to this Balmer
  continuum excess, is similar to that of the Fermi/GBM light curve. The
  electron-beam flux estimated from Fermi/GBM between 10<SUP>9</SUP> and
  10<SUP>10</SUP> erg s<SUP>−1</SUP> cm<SUP>−2</SUP> is consistent
  with the beam flux required in non-LTE radiative transfer models
  to obtain the excess of Balmer continuum emission observed in this
  IRIS spectra. <BR /> Conclusions: The low-energy input by nonthermal
  electrons above 20 keV is sufficient to produce the enhancement in the
  Balmer continuum emission. This could be explained by the topology of
  the reconnection site. The reconnection starts in a tiny bald-patch
  region, which is transformed dynamically into an X-point current
  sheet. The size of the interacting region would be below the spatial
  resolution of the instrument.

---------------------------------------------------------
Title: On the importance of Ca II photoionization by the hydrogen
    lyman transitions in solar flare models
Authors: Osborne, C. M. J.; Heinzel, P.; Kašparová, J.; Fletcher, L.
2021MNRAS.507.1972O    Altcode: 2021MNRAS.tmp.1947O; 2021arXiv210711145O
  The forward fitting of solar flare observations with
  radiation-hydrodynamic simulations is a common technique for learning
  about energy deposition and atmospheric evolution during these explosive
  events. A frequent spectral line choice for this process is Ca II
  854.2 nm due to its formation in the chromosphere and substantial
  variability. It is important to ensure that this line is accurately
  modelled to obtain the correct interpretation of observations. Here,
  we investigate the importance of photoionization of Ca II to Ca III by
  the hydrogen Lyman transitions, whilst the Lyman continuum is typically
  considered in this context in simulations, the associated bound-bound
  transitions are not. This investigation uses two RADYN flare simulations
  and reprocesses the radiative transfer using the Lightweaver framework
  which accounts for the overlapping of all active transitions. The
  Ca II 854.2 nm line profiles are found to vary significantly due to
  photoionization by the Lyman lines, showing notably different shapes
  and even reversed asymmetries. Finally, we investigate to what extent
  these effects modify the energy balance of the simulation and the
  implications on future radiation-hydrodynamic simulations. There
  is found to be a 10-15 per cent change in detailed optically thick
  radiative losses from considering these photoionization effects on
  the calcium lines in the two simulations presented, demonstrating the
  importance of considering these effects in a self-consistent way.

---------------------------------------------------------
Title: VizieR Online Data Catalog: Quiet-Sun MgII h &amp; k line
    profiles from IRIS (Gunar+, 2021)
Authors: Gunar, S.; Koza, J.; Schwartz, P.; Heinzel, P.; Liu, W.
2021yCat..22550016G    Altcode:
  Since its launch, the Interface Region Imaging Spectrograph (IRIS)
  commenced a quasi-regular acquisition of maps of the entire solar
  disk in both NUV and FUV spectral ranges. At the time of writing,
  the archive of the IRIS full-Sun mosaics contained 91 observations
  spanning the period from 2013 September 30 to 2020 October 19 which
  cover two spectral windows of +/-1.75Å centered at 2803.53Å (MgII h)
  and 2796.35Å (MgII k). <P />(4 data files).

---------------------------------------------------------
Title: Exploring the Solar Wind from Its Source on the Corona into
    the Inner Heliosphere during the First Solar Orbiter-Parker Solar
    Probe Quadrature
Authors: Telloni, Daniele; Andretta, Vincenzo; Antonucci, Ester;
   Bemporad, Alessandro; Capuano, Giuseppe E.; Fineschi, Silvano;
   Giordano, Silvio; Habbal, Shadia; Perrone, Denise; Pinto, Rui F.;
   Sorriso-Valvo, Luca; Spadaro, Daniele; Susino, Roberto; Woodham, Lloyd
   D.; Zank, Gary P.; Romoli, Marco; Bale, Stuart D.; Kasper, Justin C.;
   Auchère, Frédéric; Bruno, Roberto; Capobianco, Gerardo; Case,
   Anthony W.; Casini, Chiara; Casti, Marta; Chioetto, Paolo; Corso,
   Alain J.; Da Deppo, Vania; De Leo, Yara; Dudok de Wit, Thierry;
   Frassati, Federica; Frassetto, Fabio; Goetz, Keith; Guglielmino,
   Salvo L.; Harvey, Peter R.; Heinzel, Petr; Jerse, Giovanna; Korreck,
   Kelly E.; Landini, Federico; Larson, Davin; Liberatore, Alessandro;
   Livi, Roberto; MacDowall, Robert J.; Magli, Enrico; Malaspina, David
   M.; Massone, Giuseppe; Messerotti, Mauro; Moses, John D.; Naletto,
   Giampiero; Nicolini, Gianalfredo; Nisticò, Giuseppe; Panasenco,
   Olga; Pancrazzi, Maurizio; Pelizzo, Maria G.; Pulupa, Marc; Reale,
   Fabio; Romano, Paolo; Sasso, Clementina; Schühle, Udo; Stangalini,
   Marco; Stevens, Michael L.; Strachan, Leonard; Straus, Thomas; Teriaca,
   Luca; Uslenghi, Michela; Velli, Marco; Verscharen, Daniel; Volpicelli,
   Cosimo A.; Whittlesey, Phyllis; Zangrilli, Luca; Zimbardo, Gaetano;
   Zuppella, Paola
2021ApJ...920L..14T    Altcode: 2021arXiv211011031T
  This Letter addresses the first Solar Orbiter (SO)-Parker Solar
  Probe (PSP) quadrature, occurring on 2021 January 18 to investigate
  the evolution of solar wind from the extended corona to the inner
  heliosphere. Assuming ballistic propagation, the same plasma volume
  observed remotely in the corona at altitudes between 3.5 and 6.3
  solar radii above the solar limb with the Metis coronagraph on SO
  can be tracked to PSP, orbiting at 0.1 au, thus allowing the local
  properties of the solar wind to be linked to the coronal source region
  from where it originated. Thanks to the close approach of PSP to the
  Sun and the simultaneous Metis observation of the solar corona, the
  flow-aligned magnetic field and the bulk kinetic energy flux density
  can be empirically inferred along the coronal current sheet with an
  unprecedented accuracy, allowing in particular estimation of the Alfvén
  radius at 8.7 solar radii during the time of this event. This is thus
  the very first study of the same solar wind plasma as it expands from
  the sub-Alfvénic solar corona to just above the Alfvén surface.

---------------------------------------------------------
Title: Quiet-Sun Mg II h and k Line Profiles Derived from IRIS
    Full-Sun Mosaics. I. Reference Profiles and Center-to-limb Variation
Authors: Gunár, Stanislav; Koza, Július; Schwartz, Pavol; Heinzel,
   Petr; Liu, Wenjuan
2021ApJS..255...16G    Altcode:
  We derived high-precision reference profiles of the Mg II h and k
  lines that represent the quiet Sun during a minimum of the solar
  activity. To do so, we used the broad catalog of full-Sun mosaics
  obtained by the Interface Region Imaging Spectrograph (IRIS). To
  minimize the influence of the local variations due to the on-disk
  solar features and to achieve low levels of uncertainties, we used
  12 IRIS full-Sun mosaics without sunspots or other significant signs
  of solar activity. These mosaics were obtained between 2019 April and
  2020 September in the near-ultraviolet spectral range. In this paper,
  we present the disk-averaged reference profiles of Mg II h and Mg II
  k lines, together with a series of reference profiles spanning the
  distance between the disk center and the solar limb. These series of
  profiles offer a detailed representation of the center-to-limb variation
  of both Mg II h and Mg II k lines. The reference Mg II h and k line
  profiles provided in this paper can be used as the incident radiation
  boundary condition for radiative-transfer modeling of prominences,
  spicules, and other coronal and chromospheric structures.

---------------------------------------------------------
Title: In-flight optical performance assessment for the Metis solar
    coronagraph
Authors: Da Deppo, Vania; Chioetto, Paolo; Andretta, Vincenzo; Casini,
   Chiara; Frassetto, Fabio; Slemer, Alessandra; Zuppella, Paola; Romoli,
   Marco; Fineschi, Silvano; Heinzel, Petr; Naletto, Giampiero; Nicolini,
   Gianalfredo; Spadaro, Daniele; Stangalini, Marco; Teriaca, Luca;
   Bemporad, Alessandro; Casti, Marta; Fabi, Michele; Grimani, Catia;
   Heerlein, Klaus; Jerse, Giovanna; Landini, Federico; Liberatore,
   Alessandro; Magli, Enrico; Melich, Radek; Pancrazzi, Maurizio; Pelizzo,
   Maria-G.; Romano, Paolo; Sasso, Clementina; Straus, Thomas; Susino,
   Roberto; Uslenghi, Michela; Volpicelli, Cosimo Antonio
2021SPIE11852E..10D    Altcode:
  Metis is a multi-wavelength coronagraph onboard the European Space
  Agency (ESA) Solar Orbiter mission. The instrument features an
  innovative instrument design conceived for simultaneously imaging the
  Sun's corona in the visible and ultraviolet range. The Metis visible
  channel employs broad-band, polarized imaging of the visible K-corona,
  while the UV one uses narrow-band imaging at the HI Ly 􀄮, i.e. 121.6
  nm. During the commissioning different acquisitions and activities,
  performed with both the Metis channels, have been carried out with the
  aim to check the functioning and the performance of the instrument. In
  particular, specific observations of stars have been devised to assess
  the optical alignment of the telescope and to derive the instrument
  optical parameters such as focal length, PSF and possibly check the
  optical distortion and the vignetting function. In this paper, the
  preliminary results obtained for the PSF of both channels and the
  determination of the scale for the visible channel will be described
  and discussed. The in-flight obtained data will be compared to those
  obtained on-ground during the calibration campaign.

---------------------------------------------------------
Title: On-ground flat-field calibration of the Metis coronagraph
    onboard the Solar Orbiter ESA mission
Authors: Casini, C.; Da Deppo, V.; Zuppella, P.; Chioetto, P.; Slemer,
   A.; Frassetto, F.; Romoli, M.; Landini, F.; Pancrazzi, M.; Andretta,
   V.; De Leo, Y.; Bemporad, A.; Fabi, M.; Fineschi, S.; Frassati, F.;
   Grimani, C.; Jerse, G.; Heerlein, K.; Liberatore, A.; Magli, E.;
   Naletto, G.; Nicolini, G.; Pelizzo, M. G.; Romano, P.; Sasso, C.;
   Spadaro, D.; Stangalini, M.; Straus, T.; Susino, R.; Teriaca, L.;
   Uslenghi, M.; Casti, M.; Heinzel, P.; Volpicelli, A.
2021SPIE11852E..5BC    Altcode:
  Solar Orbiter, launched on February 9<SUP>th</SUP> 2020, is an
  ESA/NASA mission conceived to study the Sun. This work presents
  the embedded Metis coronagraph and its on-ground calibration in the
  580-640 nm wavelength range using a flat field panel. It provides
  a uniform illumination to evaluate the response of each pixel of
  the detector; and to characterize the Field of View (FoV) of the
  coronagraph. Different images with different exposure times were
  acquired during the on-ground calibration campaign. They were analyzed
  to verify the linearity response of the instrument and the requirements
  for the FoV: the maximum area of the sky that Metis can acquire.

---------------------------------------------------------
Title: Challenges during Metis-Solar Orbiter commissioning phase
Authors: Romoli, Marco; Andretta, Vincenzo; Bemporad, Alessandro;
   Casti, Marta; Da Deppo, Vania; De Leo, Yara; Fabi, Michele; Fineschi,
   Silvano; Frassetto, Fabio; Grimani, Catia; Heerlein, Klaus; Heinzel,
   Petr; Jerse, Giovanna; Landini, Federico; Liberatore, Alessandro;
   Magli, Enrico; Naletto, Giampiero; Nicolini, Gianalfredo; Pancrazzi,
   Maurizio; Pelizzo, Maria Guglielmina; Romano, Paolo; Sasso, Clementina;
   Schühle, Udo; Slemer, Alessandra; Spadaro, Daniele; Straus, Thomas;
   Susino, Roberto; Teriaca, Luca; Uslenghi, Michela; Volpicelli, Cosimo
   Antonio; Zupella, Paola
2021SPIE11852E..5AR    Altcode:
  Metis is the visible light and UV light imaging coronagraph on board
  the ESA-NASA mission Solar Orbiter that has been launched February 10th,
  2020, from Cape Canaveral. Scope of the mission is to study the Sun up
  close, taking high-resolution images of the Sun's poles for the first
  time, and understanding the Sun-Earth connection. Metis coronagraph
  will image the solar corona in the linearly polarized broadband visible
  radiation and in the UV HI Ly-α line from 1.6 to 3 solar radii when at
  Solar Orbiter perihelion, providing a diagnostics, with unprecedented
  temporal coverage and spatial resolution, of the structures and dynamics
  of the full corona. Solar Orbiter commissioning phase big challenge was
  Covid-19 social distancing phase that affected the way commissioning
  of a spacecraft and its payload is typically done. Metis coronagraph
  on-board Solar Orbiter had its additional challenges: to wake up and
  check the performance of the optical, electrical and thermal subsystems,
  most of them unchecked since Metis delivery to spacecraft prime, Airbus,
  in May 2017. The roadmap to the fully commissioned coronagraph is here
  described throughout the steps from the software functional test,
  the switch on of the detectors of the two channels, UV and visible,
  to the optimization of the occulting system and the characterization
  of the instrumental stray light, one of the most challenging features
  in a coronagraph.

---------------------------------------------------------
Title: In-flight calibration of Metis coronagraph on board of
    Solar Orbiter
Authors: Liberatore, A.; Fineschi, S.; Casti, M.; Capobianco, G.;
   Romoli, M.; Andretta, V.; Bemporad, A.; Da Deppo, V.; De Leo, Y.; Fabi,
   M.; Frassetto, F.; Grimani, C.; Heerlein, K.; Heinzel, P.; Jerse,
   G.; Landini, F.; Magli, E.; Naletto, G.; Nicolini, G.; Pancrazzi,
   M.; Pelizzo, M. G.; Romano, P.; Sasso, C.; Slemer, A.; Spadaro, D.;
   Straus, T.; Susino, R.; Teriaca, L.; Uslenghi, M.; Volpicelli, C. A.;
   Zuppella, P.
2021SPIE11852E..48L    Altcode:
  Metis coronagraph is one of the remote-sensing instruments of the Solar
  Orbiter mission launched at the begin of 2020. The mission profile will
  allow for the first time the remote-sensing observation of the Sun
  from a very close distance and increasing the latitude with respect
  to the ecliptic plane. In particular, Metis is aimed at the overall
  characterization and study of the solar corona and solar wind. Metis
  instrument acquires images of the solar corona in two different
  wavelengths simultaneously; ultraviolet (UV) and visible-light (VL). The
  VL channel includes a polarimeter with an electro-optically modulating
  Liquid Crystal Variable Retarder (LCVR) to measure the linearly
  polarized brighness pB) of the K-corona. This paper presents part of
  the in-flight calibration results for both wavelength channels together
  with a comparison with on-ground calibrations. The orientation of the
  K-corona linear polarization was used for the in-flight calibration
  of the Metis polarimeter. This paper describes the correction of the
  on-ground VL vignetting function after the in-flight adjustment of
  the internal occulter. The same vignetting function was adaptated to
  the UV channel.

---------------------------------------------------------
Title: IRIS observations of chromospheric heating by acoustic waves
    in solar quiet and active regions
Authors: Abbasvand, V.; Sobotka, M.; Švanda, M.; Heinzel, P.; Liu,
   W.; Mravcová, L.
2021A&A...648A..28A    Altcode: 2021arXiv210208678A
  <BR /> Aims: To study the heating of solar chromospheric magnetic and
  nonmagnetic regions by acoustic and magnetoacoustic waves, the deposited
  acoustic-energy flux derived from observations of strong chromospheric
  lines is compared with the total integrated radiative losses. <BR />
  Methods: A set of 23 quiet-Sun and weak-plage regions were observed in
  the Mg II k and h lines with the Interface Region Imaging Spectrograph
  (IRIS). The deposited acoustic-energy flux was derived from Doppler
  velocities observed at two different geometrical heights corresponding
  to the middle and upper chromosphere. A set of scaled nonlocal
  thermodynamic equilibrium 1D hydrostatic semi-empirical models -
  obtained by fitting synthetic to observed line profiles - was applied
  to compute the radiative losses. The characteristics of observed waves
  were studied by means of a wavelet analysis. <BR /> Results: Observed
  waves propagate upward at supersonic speed. In the quiet chromosphere,
  the deposited acoustic flux is sufficient to balance the radiative
  losses and maintain the semi-empirical temperatures in the layers under
  study. In the active-region chromosphere, the comparison shows that
  the contribution of acoustic-energy flux to the radiative losses is
  only 10−30%. <BR /> Conclusions: Acoustic and magnetoacoustic waves
  play an important role in the chromospheric heating, depositing a main
  part of their energy in the chromosphere. Acoustic waves compensate
  for a substantial fraction of the chromospheric radiative losses in
  quiet regions. In active regions, their contribution is too small to
  balance the radiative losses and the chromosphere has to be heated by
  other mechanisms.

---------------------------------------------------------
Title: Constraining stellar CME occurrence with optical spectroscopy
Authors: Odert, Petra; Leitzinger, Martin; Guenther, Eike W.;
   Heinzel, Petr
2021csss.confE..96O    Altcode:
  Our knowledge on coronal mass ejections (CMEs) on stars other than the
  Sun is still sparse. Spectroscopic observations in the optical sometimes
  show asymmetrically broadened wings and/or transient extra-emissions in
  chromospheric lines during or shortly after flare events. These may be
  interpreted as signatures of prominence eruptions, which are closely
  related to CMEs on the Sun. Dedicated searches for these signatures
  have, however, mostly yielded non-detections. Here we present a
  semi-empirical model which combines predictions of intrinsic stellar
  CME rates with simple radiative transfer calculations in the Balmer
  lines. We find that typical observations have most likely been too
  short and/or they had a too low signal-to-noise ratio to detect CMEs. We
  predict the minimum observing time needed to detect CMEs in the Balmer
  lines for stars with different spectral types and activity levels.

---------------------------------------------------------
Title: Multi-thermal atmosphere of a mini-solar flare during magnetic
    reconnection observed with IRIS
Authors: Joshi, Reetika; Schmieder, Brigitte; Tei, Akiko; Aulanier,
   Guillaume; Lörinčík, Juraj; Chandra, Ramesh; Heinzel, Petr
2021A&A...645A..80J    Altcode: 2020arXiv201015401J
  Context. The Interface Region Imaging Spectrograph (IRIS) with its
  high spatial and temporal resolution facilitates exceptional plasma
  diagnostics of solar chromospheric and coronal activity during magnetic
  reconnection. <BR /> Aims: The aim of this work is to study the fine
  structure and dynamics of the plasma at a jet base forming a mini-flare
  between two emerging magnetic fluxes (EMFs) observed with IRIS and the
  Solar Dynamics Observatory instruments. <BR /> Methods: We proceed to
  a spatio-temporal analysis of IRIS spectra observed in the spectral
  ranges of Mg II, C II, and Si IV ions. Doppler velocities from Mg II
  lines were computed using a cloud model technique. <BR /> Results:
  Strong asymmetric Mg II and C II line profiles with extended blue
  wings observed at the reconnection site (jet base) are interpreted by
  the presence of two chromospheric temperature clouds: one explosive
  cloud with blueshifts at 290 km s<SUP>-1</SUP> and one cloud with
  smaller Doppler shift (around 36 km s<SUP>-1</SUP>). Simultaneously at
  the same location (jet base), strong emission of several transition
  region lines (e.g. O IV and Si IV), emission of the Mg II triplet
  lines, and absorption of identified chromospheric lines in Si IV
  broad profiles have been observed and analysed. <BR /> Conclusions:
  Such observations of IRIS line and continuum emissions allow us
  to propose a stratification model for the white light, mini-flare
  atmosphere with multiple layers of different temperatures along the
  line of sight in a reconnection current sheet. It is the first time
  that we could quantify the fast speed (possibly Alfvénic flows)
  of cool clouds ejected perpendicularly to the jet direction via the
  cloud model technique. We conjecture that the ejected clouds come from
  plasma which was trapped between the two EMFs before reconnection or
  be caused by chromospheric-temperature (cool) upflow material similar
  to a surge during reconnection. <P />Movies are available at <A
  href="https://www.aanda.org/10.1051/0004-6361/202039229/olm">https://www.aanda.org</A>

---------------------------------------------------------
Title: Spectral inversion of H-alpha and MgII lines in quiescent
    prominences
Authors: Heinzel, Petr; Schmieder, Brigitte; Ruan, Guiping; Mein,
   Pierre; Gunár, Stanislav; Jejcic, Sonja; Mein, Nicole
2021cosp...43E1764H    Altcode:
  Recent spectral analysis of simultaneous H-alpha (MSDP) and MgII
  lines (IRIS) (Guiping et al. 2019) has revealed certain bifurcation
  in resulting models. Two solutions were found from the line inversions
  using the non-LTE modeling: relatively high kinetic temperature and low
  non-thermal motions or temperatures mostly compatible with standard ones
  plus non-thermal motions of the order of 16 km/sec. Here we will present
  an improved spectral line inversion technique which clearly prefers
  the latter solution. Strong non-thermal motions are then interpreted
  as a mixture of microturbulence and the line-of-sight dynamics of
  prominence fine-structure threads. A detailed multithread modeling with
  the 2D non-LTE code and stochastic distributions of threads (position,
  dynamics) is now in progress and we will show our preliminary results.

---------------------------------------------------------
Title: Magnetic support of the solar filaments
Authors: Schmieder, Brigitte; Aulanier, Guillaume; Gunár, Stanislav;
   Dudik, Jaroslav; Heinzel, Petr
2021cosp...43E1766S    Altcode:
  The scale height in prominence is 500 km at maximum. However, non
  activated prominences can reach an altitude of 50000 km or more. Hanging
  filaments observed over the limb give the impression of quasi vertical
  structures. It was already the view in the past but reactivated by the
  movies of Hinode in Ca II line showing fuzzing vertical structures. In
  the corona it is not possible to measure the magnetic field supporting
  prominences. Only extrapolations of the photospheric magnetic field
  explain how cool plasma embedded in the dips of the magnetic field
  lines can be supported in the hot corona. I will review a few papers
  showing the distribution of the cool plasma dips and the observations
  of filaments on the disk visible in H$\alpha$ and in UV. A recent
  paper shows how a 3D extrapolation model and a radiative-transfer
  based H$\alpha$ visualization method leads to H$\alpha$ prominence
  fine structures. Finally, I will discuss the perspective effects on
  the perceived morphology of observed and modeled prominences.

---------------------------------------------------------
Title: Cool flare loops in solar and stellar coronae
Authors: Heinzel, Petr
2021cosp...43E.969H    Altcode:
  Cool structures in solar and stellar coronae may take various forms
  like prominences, cores of CMEs or cool flare loops which often exhibit
  the so-called coronal rain. In this talk we will focus on the latter
  structures which recently attracted a great attention in relation with
  largest solar flares observed during the 24th solar cycle. We will
  summarise the multi-wavelength observations of giant off-limb post-flare
  loops from September 10, 2017 and show the principally new results
  concerning their magnetic fields and overall densities. High densities
  obtained certainly require a strong magnetic field to keep the loops
  stably confined in the corona. Downflows consistent with the coronal
  rain and high non-thermal motions (the so-called microturbulence) have
  been detected. Moreover, SDO/HMI data also indicate high densities
  which would be compatible with those predicted in loops expected on
  other cool stars. These conditions are favourable for explanation of
  the continuum emission enhancements during superflares, in terms of
  the loop-arcade component. However, in order to explain the superflare
  behaviour, large loop-arcade areas are required as suggested in Heinzel
  and Shibata 2018. Finally, we will show the effect of cool stellar
  loops on the spectral line emission variations during a flare which
  seems to be an unresolved mixture of ribbon and loop emission.

---------------------------------------------------------
Title: Links between prominence/filament magnetic field and plasma:
    What can 3D WPFS models teach us?
Authors: Gunár, Stanislav; Schmieder, Brigitte; Aulanier, Guillaume;
   Heinzel, Petr; Mackay, Duncan; Dudik, Jaroslav
2021cosp...43E1769G    Altcode:
  The magnetic field constitutes the skeleton and the driving force of
  prominences/filaments. It supports the dense prominence plasma against
  gravity and insulates it from the hot, coronal environment. The
  magnetic field is also responsible for the prominence stability,
  evolution and eruptions which affect the heliosphere and ultimately
  the Earth. However, a strong imbalance exists between the numerous
  efforts in detailed modelling of prominence magnetic field and its
  understanding from observations. That is due to the complex nature of
  the direct (and indirect) observations of solar magnetic fields which
  are challenging at the best of times and even more so in prominences
  or filaments. The direct observations of the prominence magnetic
  field require high-precision spectro-polarimetric measurements and
  realistic assumptions about the plasma structure which allow us to
  infer the field configuration from its effect on the polarized light
  emergent from the observed structures. The indirect observations rely
  on the perceived location, shape and dynamics of the prominence or
  filament plasma, often using moving small-scale plasma structures
  as tracers guided by the field lines. Both methods thus rely on the
  presence of observable plasma in the magnetic field configuration,
  and on the radiation which carries the information about the in-situ
  conditions to the observer. No prominence/filament magnetic field
  measurements are made without these two additional components,
  which are sometimes an afterthought in the magnetic field models. We
  have developed 3D Whole-Prominence Fine Structure (WPFS) models to
  illuminate the links between the prominence magnetic field, its plasma
  distributed among numerous fine structures and the radiation which
  carries the information about the prominence physical conditions to
  the observer. What can we learn from these 3D models? For example,
  we can see that a small change of the magnetic field configuration
  can have a large effect on the perceived structure of prominences and
  filaments visible in the H-alpha line. Consequently, this means that
  significant changes observed in prominences or filaments do not need
  to suggest that equally large changes in the underlying magnetic field
  configuration had to occur. In another example, we see that seemingly
  incomparable differences in the morphological look of prominences (long
  horizontal fine structures versus small blobs of plasma arranged into
  more-less vertical features) may not need to imply the existence of
  radically different magnetic field configurations. Rather, they might
  simply be manifestations of projection effects that can differ greatly
  depending on the viewing angle under which we observe the naturally
  three-dimensional prominences/filaments.

---------------------------------------------------------
Title: Quiet-Sun hydrogen Lyman-α line profile derived from
    SOHO/SUMER solar-disk observations
Authors: Gunár, S.; Schwartz, P.; Koza, J.; Heinzel, P.
2020A&A...644A.109G    Altcode: 2020arXiv201101299G
  Context. The solar radiation in the Lyman-α spectral line of hydrogen
  plays a significant role in the illumination of chromospheric and
  coronal structures, such as prominences, spicules, chromospheric
  fibrils, cores of coronal mass ejections, and solar wind. Moreover,
  it is important for the investigation of the heliosphere, Earth's
  ionosphere, and the atmospheres of planets, moons, and comets. <BR />
  Aims: We derive a reference quiet-Sun Lyman-α spectral profile that
  is representative of the Lyman-α radiation from the solar disk during
  a minimum of solar activity. This profile can serve as an incident
  radiation boundary condition for the radiative transfer modelling of
  chromospheric and coronal structures. Because the solar radiation in
  the Lyman lines is not constant over time but varies significantly
  with the solar cycle, we provide a method for the adaptation of
  the incident radiation Lyman line profiles (Lyman-α and higher
  lines) to a specific date. Moreover, we analyse how the change in
  the incident radiation influences the synthetic spectra produced by
  the radiative transfer modelling. <BR /> Methods: We used SOHO/SUMER
  Lyman-α raster scans obtained without the use of the attenuator in
  various quiet-Sun regions on the solar disk. The observations were
  performed on three consecutive days (June 24, 25, and 26, 2008) during
  a period of minimum solar activity. The reference Lyman-α profile was
  obtained as a spatial average over eight available raster scans. To
  take into account the Lyman-α variation with the solar cycle, we
  used the LISIRD composite Lyman-α index. To estimate the influence
  of the change in the incident radiation in the Lyman lines on the
  results of radiative transfer models, we used a 2D prominence fine
  structure model. <BR /> Results: We present the reference quiet-Sun
  Lyman-α profile and a table of coefficients describing the variation
  of the Lyman lines with the solar cycle throughout the lifetime of
  SOHO. The analysis of the influence of the change in the incident
  radiation shows that the synthetic spectra are strongly affected by
  the modification of the incident radiation boundary condition. The
  most pronounced impact is on the central and integrated intensities
  of the Lyman lines. There, the change in the synthetic spectra can
  often have the same amplitude as the change in the incident radiation
  itself. The impact on the specific intensities in the peaks of reversed
  Lyman-line profiles is smaller but still significant. The hydrogen
  Hα line can also be considerably affected, despite the fact that
  the Hα radiation from the solar disk does not vary with the solar
  cycle. <P />Data are only available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr/">http://cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/644/A109">http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/644/A109</A>

---------------------------------------------------------
Title: IRIS Mg II Observations and Non-LTE Modeling of Off-limb
    Spicules
Authors: Tei, A.; Gunár, S.; Heinzel, P.; Okamoto, T. J.; Štěpán,
   J.; Jejčič, S.; Shibata, K.
2020AGUFMSH0010008T    Altcode:
  We investigated the off-limb spicules observed in the Mg II h and k
  spectral lines by Interface Region Imaging Spectrograph (IRIS) in a
  solar polar coronal hole. We analyzed the large data set of obtained
  spectra to extract quantitative information about the line intensities,
  line shifts, and line widths. The observed Mg II line profiles are
  broad and double peaked at lower altitudes, broad but flat topped
  at middle altitudes, and narrow and single peaked with the largest
  Doppler shifts at higher altitudes. We used one-dimensional non-LTE
  vertical slab models (i.e., models that consider departures from local
  thermodynamic equilibrium) in single-slab and multi-slab configurations
  to interpret the observations and to investigate how a superposition
  of spicules along a line of sight (LOS) affects the synthetic Mg II
  line profiles. The employed multi-slab models are either static,
  i.e., without any LOS velocities, or assume randomly assigned LOS
  velocities of individual slabs, representing the spicule dynamics. We
  performed such single-slab and multi-slab modeling for a broad set of
  model input parameters and examined the dependence of the Mg II line
  profiles on these parameters. In this presentation, we demonstrate that
  the observed line widths of the Mg h and k line profiles are strongly
  affected by the presence of multiple spicules along the LOS. We also
  show that the profiles obtained at higher altitudes can be reproduced
  by single-slab models representing individual spicules. We found that
  the multi-slab model with a random distribution of the LOS velocities
  ranging from −25 to 25 km/s can well reproduce the width and the
  shape of the Mg II profiles observed at middle altitudes.

---------------------------------------------------------
Title: Metis - Solar Orbiter Topical Team on "Modelling of CME
    propagation/evolution in corona and solar wind in connection with
    Space Weather"
Authors: Bemporad, A.; Banerjee, D.; Berlicki, A.; Biondo, R.; Boe,
   B.; Calchetti, D.; Capuano, G.; De Leo, Y.; Del Moro, D.; Feng, L.;
   Foldes, R.; Frassati, F.; Frazin, R. A.; Giovannelli, L.; Giunta,
   A. S.; Heinzel, P.; Ippolito, A.; Janvier, M.; Jerse, G.; Kilpua,
   K. E. J.; Laurenza, M.; Lloveras, D.; Magdalenic, J.; Mancuso, S.;
   Messerotti, M.; Mierla, M.; Nandy, D.; Napoletano, G.; Nuevo, F.;
   Pagano, P.; Pinto, R.; Plainaki, C.; Reale, F.; Romoli, M.; Rodriguez,
   L.; Slemer, A.; Spadaro, D.; Susino, R.; Stangalini, M.; Vainio,
   R. O.; Valori, G.; Vásquez, A. M.; West, M. J.
2020AGUFMSH0360027B    Altcode:
  Despite the current availability of multi-spacecraft observations of
  Coronal Mass Ejections (CMEs) and their interplanetary counterpart
  (ICMEs), at present we still don't understand which physical phenomena
  are driving their expansion and propagation phases. This also limits
  our understanding on how CMEs (observed with remote sensing data)
  become ICMEs (observed in situ), how they interact with the background
  solar wind, and how their final geo-effectiveness can be modified
  during their interplanetary evolution. Such problems match some of
  the scientific objectives of the Solar Orbiter Science Activity Plan
  and of the Metis coronagraph. Thanks to its multi-channel capability,
  Metis (acquiring images in the visible light and at the same time in
  the UV HI Lyman-alpha emission) will really provide an unprecedented
  view of CMEs and in particular of their thermodynamic evolution. At
  closest approaches to the Sun (in the nominal mission), Metis will
  acquire high spatial resolution and/or temporal cadence multi-channel
  images of CMEs. Farther from the Sun, Metis will shed light on the
  early Interplanetary propagation of CMEs. Later on (in the extended
  mission) Metis will observe for the first time the CME/ICME propagation
  out-of-ecliptic. These novelties will be combined with the unique
  vantage point that will be offered by the Solar Orbiter spacecraft,
  and supported with valuable data acquired by other on-board remote
  sensing (e.g. SPICE, EUI, SoloHI) and in situ (e.g. EPD, MAG,
  SWA, RPW) instruments. In this contribution we present the ongoing
  activities of the Metis Topical Team on "CME/ICME propagation", (<A
  href="http://metis.oato.inaf.it/topical_teams.html">http://metis.oato.inaf.it/topical_teams.html</A>),
  an international working group recently established and gathering
  scientists from different countries, experts of both in-situ and remote
  sensing observations, as well as numerical simulations, and we summarize
  the main science objectives discussed during the last months.

---------------------------------------------------------
Title: Solar Orbiter: connecting remote sensing and in situ
    measurements
Authors: Horbury, T. S.; Auchere, F.; Antonucci, E.; Berghmans, D.;
   Bruno, R.; Carlsson, M.; del Toro Iniesta, J. C.; Fludra, A.; Harra,
   L.; Hassler, D.; Heinzel, P.; Howard, R. A.; Krucker, S.; Livi, S. A.;
   Long, D.; Louarn, P.; Maksimovic, M.; Mueller, D.; Owen, C. J.; Peter,
   H.; Rochus, P. L.; Rodriguez-Pacheco, J.; Romoli, M.; Schühle, U.;
   Solanki, S. K.; Teriaca, L.; Wimmer-Schweingruber, R. F.; Zouganelis,
   Y.; Laker, R.
2020AGUFMSH038..10H    Altcode:
  A key science goal of the Solar Orbiter mission is to make connections
  between phenomena on the Sun and their manifestations in interplanetary
  space. To that end, the spacecraft carries a carefully tailored
  payload of six remote sensing instruments and four making in situ
  measurements. During June 2020, while the spacecraft was around 0.5
  AU from the Sun, the remote sensing instruments operated for several
  days. While this was primarily an engineering activity, the resulting
  observations provided outstanding measurements and represent the ideal
  first opportunity to investigate the potential for making connections
  between the remote sensing and in situ payloads on Solar Orbiter. <P
  />We present a preliminary analysis of the available remote sensing and
  in situ observations, showing how connections can be made, and discuss
  the potential for further, more precise mapping to be performed as
  the mission progresses.

---------------------------------------------------------
Title: Observational study of chromospheric heating by acoustic waves
Authors: Abbasvand, V.; Sobotka, M.; Švanda, M.; Heinzel, P.;
   García-Rivas, M.; Denker, C.; Balthasar, H.; Verma, M.; Kontogiannis,
   I.; Koza, J.; Korda, D.; Kuckein, C.
2020A&A...642A..52A    Altcode: 2020arXiv200802688A
  <BR /> Aims: Our aim is to investigate the role of acoustic and
  magneto-acoustic waves in heating the solar chromosphere. Observations
  in strong chromospheric lines are analyzed by comparing the deposited
  acoustic-energy flux with the total integrated radiative losses. <BR
  /> Methods: Quiet-Sun and weak-plage regions were observed in the Ca
  II 854.2 nm and Hα lines with the Fast Imaging Solar Spectrograph
  (FISS) at the 1.6-m Goode Solar Telescope on 2019 October 3 and
  in the Hα and Hβ lines with the echelle spectrograph attached
  to the Vacuum Tower Telescope on 2018 December 11 and 2019 June
  6. The deposited acoustic energy flux at frequencies up to 20 mHz
  was derived from Doppler velocities observed in line centers and
  wings. Radiative losses were computed by means of a set of scaled
  non-local thermodynamic equilibrium 1D hydrostatic semi-empirical
  models obtained by fitting synthetic to observed line profiles. <BR />
  Results: In the middle chromosphere (h = 1000-1400 km), the radiative
  losses can be fully balanced by the deposited acoustic energy flux in
  a quiet-Sun region. In the upper chromosphere (h &gt; 1400 km), the
  deposited acoustic flux is small compared to the radiative losses in
  quiet as well as in plage regions. The crucial parameter determining
  the amount of deposited acoustic flux is the gas density at a given
  height. <BR /> Conclusions: The acoustic energy flux is efficiently
  deposited in the middle chromosphere, where the density of gas is
  sufficiently high. About 90% of the available acoustic energy flux in
  the quiet-Sun region is deposited in these layers, and thus it is a
  major contributor to the radiative losses of the middle chromosphere. In
  the upper chromosphere, the deposited acoustic flux is too low, so that
  other heating mechanisms have to act to balance the radiative cooling.

---------------------------------------------------------
Title: VizieR Online Data Catalog: Quiet-sun hydrogen Lyman-alpha
    line profile (Gunar+, 2020)
Authors: Gunar, S.; Schwartz, P.; Koza, J.; Heinzel, P.
2020yCat..36440109G    Altcode:
  The reference quiet-Sun Lyman-alpha profile obtained as an average
  over eight SOHO/SUMER raster scans obtained between 2008/06/24
  and 2008/06/26. The central wavelength lambda<SUB>0</SUB> of the
  Lyman-alpha line is 1215.67Å (121.567nm). <P />The symmetrized
  reference quiet-Sun Lyman-alpha profile obtained by symmetrization of
  the full profile from Table A1. Only the right half of the profile
  is provided. The central wavelength lambda<SUB>0</SUB> of the
  Lyman-alpha line is 1215.67Å (121.567nm). <P />table B1 ~List of
  coefficients describing the variation of the solar radiation in the
  Lyman-alpha and higher Lyman lines. The coefficients were derived from
  400-day averaged LISIRD Lyman-alpha composite index (Machol et al.,
  2019E&amp;SS....6.2263M). We provide coefficients for selected dates
  throughout the lifetime of SOHO. Coefficients for the Lyman-alpha line
  are computed with respect to the date 2008/06/25. Coefficients for the
  higher Lyman lines are computed with respect to the date 1996/05/15
  used in Warren et al. (1998ApJS..119..105W). <P />(3 data files).

---------------------------------------------------------
Title: Metis: the Solar Orbiter visible light and ultraviolet
    coronal imager
Authors: Antonucci, Ester; Romoli, Marco; Andretta, Vincenzo; Fineschi,
   Silvano; Heinzel, Petr; Moses, J. Daniel; Naletto, Giampiero; Nicolini,
   Gianalfredo; Spadaro, Daniele; Teriaca, Luca; Berlicki, Arkadiusz;
   Capobianco, Gerardo; Crescenzio, Giuseppe; Da Deppo, Vania; Focardi,
   Mauro; Frassetto, Fabio; Heerlein, Klaus; Landini, Federico; Magli,
   Enrico; Marco Malvezzi, Andrea; Massone, Giuseppe; Melich, Radek;
   Nicolosi, Piergiorgio; Noci, Giancarlo; Pancrazzi, Maurizio; Pelizzo,
   Maria G.; Poletto, Luca; Sasso, Clementina; Schühle, Udo; Solanki,
   Sami K.; Strachan, Leonard; Susino, Roberto; Tondello, Giuseppe;
   Uslenghi, Michela; Woch, Joachim; Abbo, Lucia; Bemporad, Alessandro;
   Casti, Marta; Dolei, Sergio; Grimani, Catia; Messerotti, Mauro;
   Ricci, Marco; Straus, Thomas; Telloni, Daniele; Zuppella, Paola;
   Auchère, Frederic; Bruno, Roberto; Ciaravella, Angela; Corso,
   Alain J.; Alvarez Copano, Miguel; Aznar Cuadrado, Regina; D'Amicis,
   Raffaella; Enge, Reiner; Gravina, Alessio; Jejčič, Sonja; Lamy,
   Philippe; Lanzafame, Alessandro; Meierdierks, Thimo; Papagiannaki,
   Ioanna; Peter, Hardi; Fernandez Rico, German; Giday Sertsu, Mewael;
   Staub, Jan; Tsinganos, Kanaris; Velli, Marco; Ventura, Rita; Verroi,
   Enrico; Vial, Jean-Claude; Vives, Sebastien; Volpicelli, Antonio;
   Werner, Stephan; Zerr, Andreas; Negri, Barbara; Castronuovo, Marco;
   Gabrielli, Alessandro; Bertacin, Roberto; Carpentiero, Rita; Natalucci,
   Silvia; Marliani, Filippo; Cesa, Marco; Laget, Philippe; Morea, Danilo;
   Pieraccini, Stefano; Radaelli, Paolo; Sandri, Paolo; Sarra, Paolo;
   Cesare, Stefano; Del Forno, Felice; Massa, Ernesto; Montabone, Mauro;
   Mottini, Sergio; Quattropani, Daniele; Schillaci, Tiziano; Boccardo,
   Roberto; Brando, Rosario; Pandi, Arianna; Baietto, Cristian; Bertone,
   Riccardo; Alvarez-Herrero, Alberto; García Parejo, Pilar; Cebollero,
   María; Amoruso, Mauro; Centonze, Vito
2020A&A...642A..10A    Altcode: 2019arXiv191108462A
  <BR /> Aims: Metis is the first solar coronagraph designed for a
  space mission and is capable of performing simultaneous imaging of the
  off-limb solar corona in both visible and UV light. The observations
  obtained with Metis aboard the Solar Orbiter ESA-NASA observatory
  will enable us to diagnose, with unprecedented temporal coverage and
  spatial resolution, the structures and dynamics of the full corona
  in a square field of view (FoV) of ±2.9° in width, with an inner
  circular FoV at 1.6°, thus spanning the solar atmosphere from 1.7
  R<SUB>⊙</SUB> to about 9 R<SUB>⊙</SUB>, owing to the eccentricity
  of the spacecraft orbit. Due to the uniqueness of the Solar Orbiter
  mission profile, Metis will be able to observe the solar corona
  from a close (0.28 AU, at the closest perihelion) vantage point,
  achieving increasing out-of-ecliptic views with the increase of the
  orbit inclination over time. Moreover, observations near perihelion,
  during the phase of lower rotational velocity of the solar surface
  relative to the spacecraft, allow longer-term studies of the off-limb
  coronal features, thus finally disentangling their intrinsic evolution
  from effects due to solar rotation. <BR /> Methods: Thanks to a novel
  occultation design and a combination of a UV interference coating of
  the mirrors and a spectral bandpass filter, Metis images the solar
  corona simultaneously in the visible light band, between 580 and 640
  nm, and in the UV H I Lyman-α line at 121.6 nm. The visible light
  channel also includes a broadband polarimeter able to observe the
  linearly polarised component of the K corona. The coronal images in
  both the UV H I Lyman-α and polarised visible light are obtained at
  high spatial resolution with a spatial scale down to about 2000 km
  and 15 000 km at perihelion, in the cases of the visible and UV light,
  respectively. A temporal resolution down to 1 s can be achieved when
  observing coronal fluctuations in visible light. <BR /> Results: The
  Metis measurements, obtained from different latitudes, will allow for
  complete characterisation of the main physical parameters and dynamics
  of the electron and neutral hydrogen/proton plasma components of the
  corona in the region where the solar wind undergoes the acceleration
  process and where the onset and initial propagation of coronal mass
  ejections (CMEs) take place. The near-Sun multi-wavelength coronal
  imaging performed with Metis, combined with the unique opportunities
  offered by the Solar Orbiter mission, can effectively address crucial
  issues of solar physics such as: the origin and heating/acceleration
  of the fast and slow solar wind streams; the origin, acceleration,
  and transport of the solar energetic particles; and the transient
  ejection of coronal mass and its evolution in the inner heliosphere,
  thus significantly improving our understanding of the region connecting
  the Sun to the heliosphere and of the processes generating and driving
  the solar wind and coronal mass ejections. <BR /> Conclusions: This
  paper presents the scientific objectives and requirements, the overall
  optical design of the Metis instrument, the thermo-mechanical design,
  and the processing and power unit; reports on the results of the
  campaigns dedicated to integration, alignment, and tests, and to
  the characterisation of the instrument performance; describes the
  operation concept, data handling, and software tools; and, finally,
  the diagnostic techniques to be applied to the data, as well as a brief
  description of the expected scientific products. The performance of the
  instrument measured during calibrations ensures that the scientific
  objectives of Metis can be pursued with success. <P />Metis website:
  <A href="http://metis.oato.inaf.it">http://metis.oato.inaf.it</A>

---------------------------------------------------------
Title: On the Possibility of Detecting Helium D3 Line Polarization
    with Metis
Authors: Heinzel, Petr; Štěpán, Jiři; Bemporad, Alessandro;
   Fineschi, Silvano; Jejčič, Sonja; Labrosse, Nicolas; Susino, Roberto
2020ApJ...900....8H    Altcode: 2020arXiv200708940H
  Metis, the space coronagraph on board the Solar Orbiter, offers us
  new capabilities for studying eruptive prominences and coronal mass
  ejections (CMEs). Its two spectral channels, hydrogen Lα and visible
  light (VL), will provide for the first time coaligned and cotemporal
  images to study dynamics and plasma properties of CMEs. Moreover,
  with the VL channel (580-640 nm) we find an exciting possibility
  to detect the helium D<SUB>3</SUB> line (587.73 nm) and its linear
  polarization. The aim of this study is to predict the diagnostic
  potential of this line regarding the CME thermal and magnetic
  structure. For a grid of models we first compute the intensity of the
  D<SUB>3</SUB> line together with VL continuum intensity due to Thomson
  scattering on core electrons. We show that the Metis VL channel will
  detect a mixture of both, with predominance of the helium emission at
  intermediate temperatures between 30 and 50,000 K. Then we use the
  code HAZEL to compute the degree of linear polarization detectable
  in the VL channel. This is a mixture of D<SUB>3</SUB> scattering
  polarization and continuum polarization. The former one is lowered in
  the presence of a magnetic field and the polarization axis is rotated
  (Hanle effect). Metis has the capability of measuring Q/I and U/I
  polarization degrees and we show their dependence on temperature and
  magnetic field. At T = 30,000 K we find a significant lowering of
  Q/I which is due to strongly enhanced D<SUB>3</SUB> line emission,
  while depolarization at 10 G amounts roughly to 10%.

---------------------------------------------------------
Title: Spectral Characteristics and Formation Height of Off-limb
    Flare Ribbons
Authors: Kuridze, David; Mathioudakis, Mihalis; Heinzel, Petr; Koza,
   Július; Morgan, Huw; Oliver, Ramon; Kowalski, Adam F.; Allred, Joel C.
2020ApJ...896..120K    Altcode: 2020arXiv200510924K
  Flare ribbons are bright manifestations of flare energy dissipation
  in the lower solar atmosphere. For the first time, we report on
  high-resolution imaging spectroscopy observations of flare ribbons
  situated off limb in the Hβ and Ca II 8542 Å lines and make a detailed
  comparison with radiative hydrodynamic simulations. Observations of
  the X8.2 class solar flare SOL 2017-09-10T16:06 UT obtained with the
  Swedish Solar Telescope reveal bright horizontal emission layers
  in Hβ line-wing images located near the footpoints of the flare
  loops. The apparent separation between the ribbon observed in the Hβ
  wing and the nominal photospheric limb is about 300-500 km. The Ca II
  8542 Å line-wing images show much fainter ribbon emissions located
  right on the edge of the limb, without clear separation from the
  limb. RADYN models are used to investigate synthetic spectral line
  profiles for the flaring atmosphere, and good agreement is found
  with the observations. The simulations show that, toward the limb,
  where the line of sight is substantially oblique with respect to the
  vertical direction, the flaring atmosphere model reproduces the high
  contrast of the off-limb Hβ ribbons and their significant elevation
  above the photosphere. The ribbons in the Ca II 8542 Å line-wing
  images are located deeper in the lower solar atmosphere with a lower
  contrast. A comparison of the height deposition of electron beam energy
  and the intensity contribution function shows that the Hβ line-wing
  intensities can be a useful tracer of flare energy deposition in the
  lower solar atmosphere.

---------------------------------------------------------
Title: Signatures of Helium Continuum in Cool Flare Loops Observed
    by SDO/AIA
Authors: Heinzel, Petr; Schwartz, Pavol; Lörinčík, Juraj; Koza,
   Július; Jejčič, Sonja; Kuridze, David
2020ApJ...896L..35H    Altcode: 2020arXiv200600574H
  We present an analysis of off-limb cool flare loops observed by the
  Solar Dynamics Observatory (SDO)/Atmospheric Imaging Assembly (AIA)
  during the gradual phase of SOL2017-09-10T16:06 X8.2-class flare. In the
  extreme-ultraviolet (EUV) channels starting from the 335 Å one, cool
  loops appear as dark structures against the bright loop arcade. These
  dark structures were precisely coaligned (spatially and temporally)
  with loops observed by Swedish Solar Telescope (SST) in emission lines
  of hydrogen and ionized calcium. A recently published semi-empirical
  model of cool loops based on SST observations serves to predict the
  level of hydrogen and helium recombination continua. The continua were
  synthesized using an approximate non-LTE (I.e., departures from local
  thermodynamic equilibrium) approach and theoretical spectra were then
  transformed to AIA signals. Comparison with signals detected inside
  the dark loops shows that only in AIA 211 Å channel the computed
  level of recombination continua is consistent with observations for
  some models, while in all other channels that are more distant from
  the continua edges the synthetic continuum is far too low. In analogy
  with on-disk observations of flares we interpret the surplus emission
  as due to numerous EUV lines emitted from hot but faint loops in front
  of the cool ones. Finally we briefly comment on failure of the standard
  absorption model when used for analysis of the dark-loop brightness.

---------------------------------------------------------
Title: Optical design of the multi-wavelength imaging coronagraph
    Metis for the solar orbiter mission
Authors: Fineschi, S.; Naletto, G.; Romoli, M.; Da Deppo, V.;
   Antonucci, E.; Moses, D.; Malvezzi, A. M.; Nicolini, G.; Spadaro,
   D.; Teriaca, L.; Andretta, V.; Capobianco, G.; Crescenzio, G.;
   Focardi, M.; Frassetto, F.; Landini, F.; Massone, G.; Melich, R.;
   Nicolosi, P.; Pancrazzi, M.; Pelizzo, M. G.; Poletto, L.; Schühle,
   U.; Uslenghi, M.; Vives, S.; Solanki, S. K.; Heinzel, P.; Berlicki,
   A.; Cesare, S.; Morea, D.; Mottini, S.; Sandri, P.; Alvarez-Herrero,
   A.; Castronuovo, M.
2020ExA....49..239F    Altcode: 2020ExA...tmp...14F
  This paper describes the innovative optical design of the Metis
  coronagraph for the Solar Orbiter ESA-NASA mission. Metis is a
  multi-wavelength, externally occulted telescope for the imaging
  of the solar corona in both the visible and ultraviolet wavelength
  ranges. Metis adopts a novel occultation scheme for the solar disk,
  that we named "inverse external occulter", for reducing the extremely
  high thermal load on the instrument at the spacecraft perihelion. The
  core of the Metis optical design is an aplanatic Gregorian telescope
  common to both the visible and ultraviolet channels. A suitable
  dichroic beam-splitter, optimized for transmitting a narrow-band in
  the ultraviolet (121.6 nm, HI Lyman-α) and reflecting a broadband
  in the visible (580-640 nm) spectral range, is used to separate the
  two optical paths. Along the visible light optical path, a liquid
  crystal electro-optical modulator, used for the first time in space,
  allows making polarimetric measurements.

---------------------------------------------------------
Title: Stellar coronal mass ejections - II. Constraints from
    spectroscopic observations
Authors: Odert, P.; Leitzinger, M.; Guenther, E. W.; Heinzel, P.
2020MNRAS.494.3766O    Altcode: 2020MNRAS.tmp.1176O; 2020arXiv200404063O
  Detections of stellar coronal mass ejections (CMEs) are still
  rare. Observations of strong Balmer line asymmetries during flare
  events have been interpreted as being caused by CMEs. Here, we aim to
  estimate the maximum possible Balmer line fluxes expected from CMEs
  to infer their detectability in spectroscopic observations. Moreover,
  we use these results together with a model of intrinsic CME rates to
  infer the potentially observable CME rates for stars of different
  spectral types under various observing conditions, as well as the
  minimum required observing time to detect stellar CMEs in Balmer
  lines. We find that generally CME detection is favoured for mid-
  to late-type M dwarfs, as they require the lowest signal-to-noise
  ratio for CME detection, and the fraction of observable-to-intrinsic
  CMEs is largest. They may require, however, longer observing times
  than stars of earlier spectral types at the same activity level,
  as their predicted intrinsic CME rates are lower. CME detections
  are generally favoured for stars close to the saturation regime,
  because they are expected to have the highest intrinsic rates; the
  predicted minimum observing time to detect CMEs on just moderately
  active stars is already &gt;100 h. By comparison with spectroscopic
  data sets including detections as well as non-detections of CMEs,
  we find that our modelled maximum observable CME rates are generally
  consistent with these observations on adopting parameters within the
  ranges determined by observations of solar and stellar prominences.

---------------------------------------------------------
Title: Chromospheric Heating by Acoustic Waves Compared to Radiative
    Cooling. II. Revised Grid of Models
Authors: Abbasvand, Vahid; Sobotka, Michal; Heinzel, Petr; Švanda,
   Michal; Jurčák, Jan; del Moro, Dario; Berrilli, Francesco
2020ApJ...890...22A    Altcode: 2020arXiv200103413A
  Acoustic and magnetoacoustic waves are considered to be possible
  agents of chromospheric heating. We present a comparison of deposited
  acoustic energy flux with total integrated radiative losses in the
  middle chromosphere of the quiet Sun and a weak plage. The comparison
  is based on a consistent set of high-resolution observations acquired
  by the Interferometric Bidimensional Spectrometer instrument in the
  Ca II 854.2 nm line. The deposited acoustic-flux energy is derived
  from Doppler velocities observed in the line core and a set of 1737
  non-local thermodynamic equilibrium 1D hydrostatic semi-empirical
  models, which also provide the radiative losses. The models are obtained
  by scaling the temperature and column mass of five initial models by
  Vernazza et al. (1981; VAL) B-F to get the best fit of synthetic to
  observed profiles. We find that the deposited acoustic-flux energy in
  the quiet-Sun chromosphere balances 30%-50% of the energy released by
  radiation. In the plage, it contributes by 50%-60% in locations with
  vertical magnetic field and 70%-90% in regions where the magnetic
  field is inclined more than 50° to the solar surface normal.

---------------------------------------------------------
Title: IRIS Mg II Observations and Non-LTE Modeling of Off-limb
    Spicules in a Solar Polar Coronal Hole
Authors: Tei, Akiko; Gunár, Stanislav; Heinzel, Petr; Okamoto,
   Takenori J.; Štěpán, Jiří; Jejčič, Sonja; Shibata, Kazunari
2020ApJ...888...42T    Altcode: 2019arXiv191112243T
  We investigated the off-limb spicules observed in the Mg II h and k
  lines by IRIS in a solar polar coronal hole. We analyzed the large data
  set of obtained spectra to extract quantitative information about the
  line intensities, shifts, and widths. The observed Mg II line profiles
  are broad and double peaked at lower altitudes, broad but flat topped
  at middle altitudes, and narrow and single peaked with the largest
  Doppler shifts at higher altitudes. We use one-dimensional non-LTE
  vertical slab models (I.e., models that consider departures from local
  thermodynamic equilibrium) in single-slab and multi-slab configurations
  to interpret the observations and to investigate how a superposition
  of spicules along the line of sight (LOS) affects the synthetic Mg
  II line profiles. The used multi-slab models either are static, I.e.,
  without any LOS velocities, or assume randomly assigned LOS velocities
  of individual slabs, representing the spicule dynamics. We conducted
  such single-slab and multi-slab modeling for a broad set of model
  input parameters and showed the dependence of the Mg II line profiles
  on these parameters. We demonstrated that the observed line widths
  of the h and k line profiles are strongly affected by the presence
  of multiple spicules along the LOS. We later showed that the profiles
  obtained at higher altitudes can be reproduced by single-slab models
  representing individual spicules. We found that the multi-slab model
  with a random distribution of the LOS velocities ranging from -25 to
  25 km s<SUP>-1</SUP> can well reproduce the width and the shape of Mg
  II profiles observed at middle altitudes.

---------------------------------------------------------
Title: Analysis of the Quasi-Periodic Pulsations in the X9.3 and X8.3
    Flares on 6 and 10 September 2017 Observed by SDO/EVE, PROBA2/LYRA
    and MAVEN/EUVM
Authors: Dominique, M.; Zhukov, A.; Thiemann, E.; Dolla, L.; Heinzel,
   P.; Wauters, L.; Dammasch, I. E.
2019AGUFMSH13D3422D    Altcode:
  Quasi-periodic pulsations (QPPs) refer to nearly-periodic oscillations
  that are often observed in irradiance time series during most solar
  flares and have also been reported in several stellar flares. Two
  families of mechanisms are usually invoked to explain QPPs: MHD
  waves and quasi-periodic particle acceleration. In both cases, QPPs
  could inform us on the conditions in which flares happen. The two
  strongest flares of the current solar cycle, i.e. the X9.3 flare on
  6 September 2017 and the off-limb X8.3 flare that occurred four days
  later, have been observed by two SXR-to-UV radiometers: SDO/EVE and
  PROBA2/LYRA. These two flares were produced in similar conditions by
  the same active region. However, if QPPs with periods between 1 and
  100 s were clearly detected in the LYRA and EVE time series during
  the first event, this was not the case during the second event. To
  understand what causes this difference between the two flares, we
  involve the observations by a third instrument: MAVEN/EUVM orbiting
  Mars. We will compare the observations by the three instruments and
  see how this can shed some light on the QPP phenomenon.

---------------------------------------------------------
Title: Diagnostics of the Prominence Plasma from Hα and Mg II
    Spectral Observations
Authors: Ruan, Guiping; Jejčič, Sonja; Schmieder, Brigitte; Mein,
   Pierre; Mein, Nicole; Heinzel, Petr; Gunár, Stanislav; Chen, Yao
2019ApJ...886..134R    Altcode:
  The goal of this paper is to derive the physical conditions of the
  prominence observed on 2017 March 30. To do so, we use a unique set
  of data in Mg II lines obtained with the space-borne Interface Region
  Imaging Spectrograph (IRIS) and in Hα line with the ground-based
  Multi-Channel Subtractive Double Pass spectrograph operating at the
  Meudon solar tower. Here, we analyze the prominence spectra of Mg
  II h and k lines, and the Hα line in the part of the prominence
  which is visible in both sets of lines. We compute a grid of 1D
  NLTE (i.e., departures from the local thermodynamical equilibrium)
  models providing synthetic spectra of Mg II k and h, and Hα lines
  in a large space of model input parameters (temperature, density,
  pressure, and microturbulent velocity). We compare Mg II and Hα
  line profiles observed in 75 positions of the prominence with the
  synthetic profiles from the grid of models. These models allow us
  to compute the relationships between the integrated intensities
  and between the optical thickness in Hα and Mg II k lines. The
  optical thickness τ <SUB>Hα </SUB> is between 0.05 and 2, and
  {τ }<SUB>Mg</SUB>{{II}}{{k}}} is between 3 and 200. We show that
  the relationship of the observed integrated intensities agrees well
  with the synthetic integrated intensities for models with a higher
  microturbulence (16 km s<SUP>-1</SUP>) and T around 8000 K, ne =
  1.5 × 10<SUP>10</SUP> cm<SUP>-3</SUP>, p = 0.05 dyne. In this case,
  large microturbulence values could be a way to take into account the
  large mixed velocities existing in the observed prominence.

---------------------------------------------------------
Title: 2D non-LTE modelling of a filament observed in the Hα line
    with the DST/IBIS spectropolarimeter
Authors: Schwartz, P.; Gunár, S.; Jenkins, J. M.; Long, D. M.;
   Heinzel, P.; Choudhary, D. P.
2019A&A...631A.146S    Altcode: 2019arXiv191003607S
  Context. We study a fragment of a large quiescent filament observed on
  May 29, 2017 by the Interferometric BIdimensional Spectropolarimeter
  (IBIS) mounted at the Dunn Solar Telescope. We focus on its quiescent
  stage prior to its eruption. <BR /> Aims: We analyse the spectral
  observations obtained in the Hα line to derive the thermodynamic
  properties of the plasma of the observed fragment of the filament. <BR
  /> Methods: We used a 2D filament model employing radiative transfer
  computations under conditions that depart from the local thermodynamic
  equilibrium. We employed a forward modelling technique in which we
  used the 2D model to produce synthetic Hα line profiles that we
  compared with the observations. We then found the set of model input
  parameters, which produces synthetic spectra with the best agreement
  with observations. <BR /> Results: Our analysis shows that one part
  of the observed fragment of the filament is cooler, denser, and
  more dynamic than its other part that is hotter, less dense, and more
  quiescent. The derived temperatures in the first part range from 6000 K
  to 10 000 K and in the latter part from 11 000 K to 14 000 K. The gas
  pressure is 0.2-0.4 dyn cm<SUP>-2</SUP> in the first part and around
  0.15 dyn cm<SUP>-2</SUP> in the latter part. The more dynamic nature
  of the first part is characterised by the line-of-sight velocities with
  absolute values of 6-7 km s<SUP>-1</SUP> and microturbulent velocities
  of 8-9 km s<SUP>-1</SUP>. On the other hand, the latter part exhibits
  line-of-sight velocities with absolute values 0-2.5 km s<SUP>-1</SUP>
  and microturbulent velocities of 4-6 km s<SUP>-1</SUP>.

---------------------------------------------------------
Title: Spectral Diagnostics of Cool Flare Loops Observed by the
    SST. I. Inversion of the Ca II 8542 Å and Hβ Lines
Authors: Koza, Július; Kuridze, David; Heinzel, Petr; Jejčič,
   Sonja; Morgan, Huw; Zapiór, Maciej
2019ApJ...885..154K    Altcode: 2019arXiv190907356K
  Flare loops form an integral part of eruptive events, being detected in
  the range of temperatures from X-rays down to cool chromospheric-like
  plasmas. While hot loops are routinely observed by the Solar Dynamics
  Observatory’s Atmospheric Imaging Assembly, cool loops seen
  off-limb are rare. In this paper we employ unique observations of
  the SOL2017-09-10T16:06 X8.2-class flare which produced an extended
  arcade of loops. The Swedish 1 m Solar Telescope made a series of
  spectral images of the cool off-limb loops in the Ca II 8542 Å and
  the hydrogen Hβ lines. Our focus is on the loop apices. Non-local
  thermal equilibrium (non-LTE; i.e., departures from LTE) spectral
  inversion is achieved through the construction of extended grids of
  models covering a realistic range of plasma parameters. The Multilevel
  Accelerated Lambda Iterations code solves the non-LTE radiative-transfer
  problem in a 1D externally illuminated slab, approximating the studied
  loop segment. Inversion of the Ca II 8542 Å and Hβ lines yields two
  similar solutions, both indicating high electron densities around 2 ×
  10<SUP>12</SUP> cm<SUP>-3</SUP> and relatively large microturbulence
  around 25 km s<SUP>-1</SUP>. These are in reasonable agreement with
  other independent studies of the same or similar events. In particular,
  the high electron densities in the range 10<SUP>12</SUP>-10<SUP>13</SUP>
  cm<SUP>-3</SUP> are consistent with those derived from the Solar
  Dynamics Observatory’s Helioseismic and Magnetic Imager white-light
  observations. The presence of such high densities in solar eruptive
  flares supports the loop interpretation of the optical continuum
  emission of stars which manifest superflares.

---------------------------------------------------------
Title: Modelling of Flare Processes: A Comparison of the Two RHD
    Codes FLARIX and RADYN
Authors: Kašparová, Jana; Carlsson, Mats; Heinzel, Petr; Varady,
   Michal
2019ASPC..519..141K    Altcode:
  We present a comparison of two autonomous, methodologically different
  radiation hydrodynamic codes, FLARIX and RADYN, and their use to model
  the solar flare processes. Both codes can model the time evolution
  of a 1D atmosphere heated by a specified process, e.g. by electron
  beams propagating from the injection site in the corona down to the
  lower atmosphere. In such a scenario time scales can be rather short
  and lead to fast heating on even sub-second time scales. Our aim is
  to compare the FLARIX and RADYN codes using exactly the same setup
  and model conditions. Although such a comparison has never been done
  successfully before for this type of codes, we will present a close
  agreement between the time evolution of the modelled atmospheric
  structure for a test case of electron beam heating.

---------------------------------------------------------
Title: Solar and Stellar Chromospheres
Authors: Heinzel, Petr; Štěpán, Jiří
2019ASPC..519...59H    Altcode:
  RADCOSMOS conference was largely devoted to many aspects of stellar
  photospheric modeling, and namely a great success of Ivan's code
  &lt;tt&gt;TLUSTY&lt;/tt&gt; was emphasized. In this short contribution
  we focus on models of solar and stellar chromospheres which are not
  in radiative equilibrium and thus require the knowledge of various
  non-radiative heating mechanisms. We desrcibe both semiempirical,
  as well as fully 3D RMHD models and mention the importance of partial
  redistribution for a proper line diagnostics. Finally, since RADCOSMOS
  was also covering topic of the polarized line transfer, we present
  here some of the latests achievements related to the solar chromosphere.

---------------------------------------------------------
Title: Modeling the Scattering Polarization of the Hydrogen Lyα
    Line Observed by CLASP in a Filament Channel
Authors: Štěpán, J.; Trujillo Bueno, J.; Gunár, S.; Heinzel, P.;
   del Pino Alemán, T.; Kano, R.; Ishikawa, R.; Narukage, N.; Bando,
   T.; Winebarger, A.; Kobayashi, K.; Auchère, F.
2019ASPC..526..165S    Altcode:
  The 400 arcsec spectrograph slit of CLASP crossed mainly quiet
  regions of the solar chromosphere, from the limb towards the solar
  disk center. Interestingly, in the CLASP slit-jaw images and in the
  SDO images of the He II line at 304 Å, we can identify a filament
  channel (FC) extending over more than 60 arcsec crossing the slit of
  the spectrograph. In order to interpret the peculiar spatial variation
  of the Q/I and U/I signals observed by CLASP in the hydrogen Lyα line
  (1216 Å), we perform multi-dimensional radiative transfer modeling
  in given filament models. In this contribution, we show the first
  results of the two-dimensional calculations we have carried out, with
  the aim of determining the filament thermal and magnetic structure by
  comparing the theoretical and the observed polarization signals. Our
  results suggest that the temperature gradients in the filament observed
  by CLASP are significantly larger than previously thought.

---------------------------------------------------------
Title: 3D Whole-Prominence Fine Structure Model as a Test Case for
    Verification and Development of Magnetic Field Inversion Techniques
Authors: Gunár, S.; Mackay, D. H.; Štěpán, J.; Heinzel, P.;
   Trujillo Bueno, J.
2019ASPC..526..159G    Altcode:
  We show the potential of a new 3D whole-prominence fine structure
  model to serve as a well-controlled yet complex environment for testing
  inversion techniques for the magnetic field inference. The realistic
  3D magnetic field and plasma environment provided by the model can
  be used for the direct synthesis of spectro-polarimetric data. Such
  synthetic data can be analyzed by advanced inversion tools and their
  results compared with the known properties provided by the model.

---------------------------------------------------------
Title: Determination of the physical properties of an erupting
    prominence from SOHO/LASCO and UVCS observations
Authors: Susino, R.; Bemporad, A.; Heinzel, P.; Jejčič, S.; Anzer,
   , U.; Dzifčáková, E.
2019NCimC..42...37S    Altcode:
  We studied the physical conditions of an erupting prominence
  observed in the core of a coronal mass ejection, using combination
  of SOHO/LASCO-C2 visible-light images and SOHO/UVCS ultraviolet
  data. Measured intensities and profiles of the neutral-hydrogen
  Lyman- α and Lyman- β lines and the 977 Å C III line were
  used together with the visible-light brightness to derive the
  geometrical and physical parameters of the prominence, such as the
  line-of-sight apparent thickness, electron column density, kinetic
  temperature, and microturbolent velocity. These parameters were used
  to constrain a non-LTE ( i.e., out of local thermodynamic equilibrium)
  radiative-transfer model of the prominence that provides the effective
  thickness, electron density, and flow velocity, in a sample of points
  selected along the prominence. The prominence can be described as a hot
  structure with low electron density and very low gas pressure compared
  to typical quiescent prominences. Intensities of the hydrogen lines
  were also used for a detailed determination of the plasma line-of-sight
  filling factor, in the two prominence points where simultaneous and
  cospatial LASCO-C2 and UVCS observations were available.

---------------------------------------------------------
Title: Chapter 5.2 - Models of Solar and Stellar Atmospheres
Authors: Heinzel, Petr
2019sgsp.book..157H    Altcode:
  This chapter addresses the basic principles of the radiative transfer
  theory and nonequilibrium plasma physics, which were developed during
  the past century and are now widely used to model solar and stellar
  atmospheres. Many key results have been obtained and new numerical
  methods developed by solar physicists; they serve as a guide for
  stellar astrophysics. We start with the basics of radiation transport
  and demonstrate the classical ideas of the nonequilibrium line formation
  using a two-level atom example. Then we summarize the equations used to
  construct standard plane-parallel models of atmospheres in hydrostatic
  and radiative equilibrium and show examples of models with different
  levels of complexity. Although such models are well-suited for modeling
  photospheres, solar and stellar chromospheres require even more advanced
  approaches. The simplest is represented by so-called semiempirical
  models; we show some classical examples for the Sun and cool stars. A
  specific class of problems concerns isolated atmospheric structures
  illuminated by solar or stellar disk radiation. Based on various
  atmospheric models, we discuss how model spectra are synthesized and
  spectral lines are actually formed. Finally, we briefly introduce the
  topic of radiation hydrodynamics as the most sophisticated tool for
  solar and stellar atmospheric modeling.

---------------------------------------------------------
Title: Blue-wing enhancement of the chromospheric Mg II h and k
    lines in a solar flare
Authors: Tei, Akiko; Sakaue, Takahito; Okamoto, Takenori J.; Kawate,
   Tomoko; Heinzel, Petr; UeNo, Satoru; Asai, Ayumi; Ichimoto, Kiyoshi;
   Shibata, Kazunari
2018PASJ...70..100T    Altcode: 2018PASJ..tmp...61T; 2018arXiv180305237T
  We performed coordinated observations of AR 12205, which showed a
  C-class flare on 2014 November 11, with the Interface Region Imaging
  Spectrograph (IRIS) and the Domeless Solar Telescope (DST) at Hida
  Observatory. Using spectral data in the Si IV 1403 Å, C II 1335 Å,
  and Mg II h and k lines from IRIS and the Ca II K, Ca II 8542 Å, and
  Hα lines from DST, we investigated a moving flare kernel during the
  flare. In the Mg II h line, the leading edge of the flare kernel showed
  an intensity enhancement in the blue wing and a smaller intensity of the
  blue-side peak (h2v) than that of the red-side one (h2r). The blueshift
  lasted for 9-48 s with a typical speed of 10.1 ± 2.6 km s<SUP>-1</SUP>,
  which was followed by a high intensity and a large redshift with a speed
  of up to 51 km s<SUP>-1</SUP> detected in the Mg II h line. The large
  redshift was a common property for all six lines, but the blueshift
  prior to it was found only in the Mg II lines. Cloud modeling of the
  Mg II h line suggests that the blue-wing enhancement with such a peak
  difference could have been caused by a chromospheric-temperature (cool)
  upflow. We discuss a scenario in which an upflow of cool plasma is
  lifted up by expanding hot plasma owing to the deep penetration of
  non-thermal electrons into the chromosphere. Furthermore, we found
  that the blueshift persisted without any subsequent redshift in the
  leading edge of the flare kernel during its decaying phase. The cause
  of such a long-lasting blueshift is also discussed.

---------------------------------------------------------
Title: Solar Ultraviolet Bursts
Authors: Young, Peter R.; Tian, Hui; Peter, Hardi; Rutten, Robert J.;
   Nelson, Chris J.; Huang, Zhenghua; Schmieder, Brigitte; Vissers, Gregal
   J. M.; Toriumi, Shin; Rouppe van der Voort, Luc H. M.; Madjarska, Maria
   S.; Danilovic, Sanja; Berlicki, Arkadiusz; Chitta, L. P.; Cheung, Mark
   C. M.; Madsen, Chad; Reardon, Kevin P.; Katsukawa, Yukio; Heinzel, Petr
2018SSRv..214..120Y    Altcode: 2018arXiv180505850Y
  The term "ultraviolet (UV) burst" is introduced to describe small,
  intense, transient brightenings in ultraviolet images of solar active
  regions. We inventorize their properties and provide a definition
  based on image sequences in transition-region lines. Coronal signatures
  are rare, and most bursts are associated with small-scale, canceling
  opposite-polarity fields in the photosphere that occur in emerging flux
  regions, moving magnetic features in sunspot moats, and sunspot light
  bridges. We also compare UV bursts with similar transition-region
  phenomena found previously in solar ultraviolet spectrometry and
  with similar phenomena at optical wavelengths, in particular Ellerman
  bombs. Akin to the latter, UV bursts are probably small-scale magnetic
  reconnection events occurring in the low atmosphere, at photospheric
  and/or chromospheric heights. Their intense emission in lines with
  optically thin formation gives unique diagnostic opportunities
  for studying the physics of magnetic reconnection in the low solar
  atmosphere. This paper is a review report from an International Space
  Science Institute team that met in 2016-2017.

---------------------------------------------------------
Title: High-density Off-limb Flare Loops Observed by SDO
Authors: Jejčič, S.; Kleint, L.; Heinzel, P.
2018ApJ...867..134J    Altcode: 2018arXiv181002431J
  The density distribution of flare loops and the mechanisms of their
  emission in the continuum are still open questions. On 2017 September
  10, a prominent loop system appeared during the gradual phase of an X8.2
  flare (SOL2017-09-10), visible in all passbands of SDO/AIA and in the
  white-light continuum of SDO/HMI. We investigate its electron density
  by taking into account all radiation processes in the flare loops,
  i.e., the Thomson continuum, hydrogen Paschen and Brackett recombination
  continua, as well as free-free continuum emission. We derive a quadratic
  function of the electron density for a given temperature and effective
  loop thickness. By absolutely calibrating SDO/HMI intensities,
  we convert the measured intensities into electron density at each
  pixel in the loops. For a grid of plausible temperatures between cool
  (6000 K) and hot (10<SUP>6</SUP> K) structures, the electron density
  is computed for representative effective thicknesses between 200 and
  20,000 km. We obtain a relatively high maximum electron density, about
  10<SUP>13</SUP> cm<SUP>-3</SUP>. At such high electron densities, the
  Thomson continuum is negligible and therefore one would not expect a
  significant polarization degree in dense loops. We conclude that the
  Paschen and Brackett recombination continua are dominant in cool flare
  loops, while the free-free continuum emission is dominant for warmer
  and hot loops.

---------------------------------------------------------
Title: Importance of the Hα Visibility and Projection Effects for
    the Interpretation of Prominence Fine-structure Observations
Authors: Gunár, Stanislav; Dudík, Jaroslav; Aulanier, Guillaume;
   Schmieder, Brigitte; Heinzel, Petr
2018ApJ...867..115G    Altcode:
  We construct a new 3D Whole-prominence Fine-structure (WPFS) model based
  on a prominence magnetic field configuration designed to qualitatively
  approximate the morphology of a quiescent prominence observed on 2010
  June 22. The model represents an entire prominence with its numerous
  fine structures formed by a prominence plasma located in dips in
  the prominence magnetic field. We use the constructed 3D model and
  employ a radiative-transfer-based Hα visualization method to analyze
  the Hα visibility of prominence fine structures and its effect
  on the perceived morphology of observed and modeled prominences. We
  qualitatively compare three techniques used for visualization of modeled
  prominences—visualizations drawing magnetic dips up to a height of
  1 pressure scale height, drawing the full extent of magnetic dips,
  and the synthetic Hα visualization—and discuss their suitability
  for direct comparison between models and observations of prominences
  and filaments. We also discuss the role of visibility of the prominence
  fine structures in the estimation of the total height of prominences,
  which may indicate the height of pre-erupting flux ropes. This
  parameter is critical for the observational determination of the
  flux-rope stability. In addition, we employ the WPFS model to assess
  the effects caused by a projection of the naturally three-dimensional
  and heterogeneous prominences onto a two-dimensional plane of the
  sky. We discuss here how the morphological structures of prominences
  differ when observed in projections from different viewing angles. We
  also discuss the shapes of the dipped magnetic field lines and the
  perceived projection of motions of prominence fine structures along
  such field lines.

---------------------------------------------------------
Title: First Detection of Solar Flare Emission in Mid-ultraviolet
    Balmer Continuum
Authors: Dominique, Marie; Zhukov, Andrei N.; Heinzel, Petr;
   Dammasch, Ingolf E.; Wauters, Laurence; Dolla, Laurent; Shestov,
   Sergei; Kretzschmar, Matthieu; Machol, Janet; Lapenta, Giovanni;
   Schmutz, Werner
2018ApJ...867L..24D    Altcode: 2018arXiv181009835D
  We present the first detection of solar flare emission at
  mid-ultraviolet wavelengths around 2000 Å by the channel 2 of the
  Large-Yield RAdiometer (LYRA) on board the PRoject for OnBoard Autonomy
  2 mission. The flare (SOL20170906) was also observed in the channel
  1 of LYRA centered at the H I Lyα line at 1216 Å, showing a clear
  non-thermal profile in both channels. The flare radiation in channel 2
  is consistent with the hydrogen Balmer continuum emission produced by an
  optically thin chromospheric slab heated up to 10,000 K. Simultaneous
  observations in channels 1 and 2 allow the separation of the line
  emission (primarily from the Lyα line) from the Balmer continuum
  emission. Together with the recent detection of the Balmer continuum
  emission in the near-ultraviolet by the Interface Region Imaging
  Spectrometer, the LYRA observations strengthen the interpretation
  of broadband flare emission as the hydrogen recombination continua
  originating in the chromosphere.

---------------------------------------------------------
Title: Statistical analysis of UV spectra of a quiescent prominence
    observed by IRIS
Authors: Jejčič, S.; Schwartz, P.; Heinzel, P.; Zapiór, M.;
   Gunár, S.
2018A&A...618A..88J    Altcode: 2018arXiv180705767J
  Context. The paper analyzes the structure and dynamics of a quiescent
  prominence that occurred on October 22, 2013 and was observed by
  several instruments including the Interface Region Imaging Spectrograph
  (IRIS). <BR /> Aims: We aim to determine the physical characteristics
  of the observed prominence using Mg II k and h (2796 and 2803 Å), C
  II (1334 and 1336 Å), and Si IV (1394 Å) lines observed by IRIS. In
  addition we study the dynamical behavior of the prominence. <BR />
  Methods: We employed the one-dimensional non-LTE (departures from the
  local thermodynamic equilibrium - LTE) modeling of Mg II lines assuming
  static isothermal-isobaric slabs. We selected a large grid of models
  with realistic input parameters expected for quiescent prominences
  (temperature, gas pressure, effective thickness, microturbulent
  velocity, height above the solar surface) and computed synthetic Mg II
  lines. The method of Scargle periodograms was used to detect possible
  prominence oscillations. <BR /> Results: We analyzed 2160 points of the
  observed prominence in five different sections along the slit averaged
  over ten pixels due to low signal to noise ratio in the C II and Si IV
  lines. We computed the integrated intensity for all studied lines, while
  the central intensity and reversal ratio was determined only for both Mg
  II and C II 1334 lines. We plotted several correlations: time evolution
  of the integrated intensities and central intensities, scatter plots
  between all combinations of line integrated intensities, and reversal
  ratio as a function of integrated intensity. We also compared Mg II
  observations with the models. Results show that more than two-thirds
  of Mg II profiles and about one-half of C II 1334 profiles are
  reversed. Profiles of Si IV are generally unreversed. The Mg II and C II
  lines are optically thick, while the Si IV line is optically thin. <BR
  /> Conclusions: The studied prominence shows no global oscillations
  in the Mg II and C II lines. Therefore, the observed time variations
  are caused by random motions of fine structures with velocities up
  to 10 km s<SUP>-1</SUP>. The observed average ratio of Mg II k to
  Mg II h line intensities can be used to determine the prominence's
  characteristic temperature. Certain disagreements between observed
  and synthetic line intensities of Mg II lines point to the necessity
  of using more complex two-dimensional multi-thread modeling in the
  future. <P />The movies associated to Figs. 1 and 7 are available at <A
  href="https://www.aanda.org/10.1051/0004-6361/201833466/olm">https://www.aanda.org</A>

---------------------------------------------------------
Title: Hot prominence detected in the core of a coronal mass
    ejection. III. Plasma filling factor from UVCS Lyman-α and Lyman-β
    observations
Authors: Susino, R.; Bemporad, A.; Jejčič, S.; Heinzel, P.
2018A&A...617A..21S    Altcode: 2018arXiv180512465S
  Context. We study an erupting prominence embedded in the core of a
  coronal mass ejection that occurred on August 2, 2000, and focus on
  deriving the plasma filling factor of the prominence. <BR /> Aims:
  We explore two methods for measuring this factor along the line of
  sight. They are based on a combination of visible-light and ultraviolet
  spectroscopic observations. <BR /> Methods: Theoretical relationships
  for resonant scattering and collisional excitation were used to evaluate
  the intensity of the neutral hydrogen Lyman-α and Lyman-β lines in
  two prominence points where simultaneous and cospatial LASCO-C2 and
  UVCS data were available. Thermodynamic and geometrical parameters
  assumed for the calculation (i.e., electron column density, kinetic
  temperature, flow velocity, chromospheric Lyα and Lyβ intensities
  and profiles, and thickness of the prominence along the line of sight)
  are provided by both observations and the results of a detailed 1D
  non-local thermal equilibrium (non-LTE) radiative-transfer model
  of the prominence, developed in our previous work. The geometrical
  filling factor was derived from comparing the calculated and measured
  intensities of the two lines. The results were then checked against the
  non-LTE model in order to verify the reliability of the methods. <BR />
  Results: The resulting filling factors are consistent with the model in
  both prominence points when the radiative and collisional components
  of the total intensity of the hydrogen lines are separated using
  the Lyα and Lyβ line intensities, which is required to estimate
  the filling factor. The exploration of the parameter space shows
  that the results are weakly sensitive to the plasma flow velocity,
  but depend more strongly on the assumed kinetic temperatures. <BR />
  Conclusions: The combination of visible-light and ultraviolet Lyα
  and Lyβ data can be used to approximately estimate the line-of-sight
  geometrical filling factor in erupting prominences, but the proposed
  technique, which is model dependent, is reliable only for emission
  that is optically thin in the lines considered, a condition that is
  not in general representative of prominence plasma.

---------------------------------------------------------
Title: 3D modelling of magnetic field and plasma structure of entire
    prominences
Authors: Gunár, Stanislav; Anzer, Ulrich; Heinzel, Petr; Mackay,
   Duncan
2018cosp...42E1315G    Altcode:
  The 3D Whole-Prominence Fine Structure (WPFS) model allows us for
  the first time to simulate entire prominences/filaments including
  their numerous fine structures. This model combines a 3D magnetic
  field configuration of an entire prominence obtained from non-linear
  force-free field simulations, with a detailed description of the
  prominence plasma. The plasma is located in magnetic dips in hydrostatic
  equilibrium and is distributed along hundreds of fine structures
  within the 3D magnetic model. The prominence plasma has realistic
  density and temperature distributions including the prominence-corona
  transition region. This allows us to produce synthetic H-alpha images
  of simulated prominences both in emission on the solar limb and in
  absorption against the solar disk (viewed as filaments) using a single
  model.Such 3D WPFS model provides us with consistent information about
  the prominence magnetic field configuration, prominence fine structure
  plasma and its radiative output. Moreover, we are able to follow the
  evolution of modeled prominences caused by changes of the underlying
  photospheric magnetic flux distribution. Thanks to these capabilities we
  can study links between the photospheric flux distribution, prominence
  magnetic field configuration, distribution and composition of the
  prominence plasma and its observable signatures. These relationships
  are important for interpretation of the observed imaging and
  spectral/spectropolarimetric data and for inference of the properties
  of the prominence magnetic field.

---------------------------------------------------------
Title: Plasma physical parameters of a prominence embedded in the
    core of a Coronal Mass Ejection
Authors: Bemporad, Alessandro; Anzer, Ulrich; Heinzel, Petr; Jejcic,
   Sonja; Susino, Roberto
2018cosp...42E.267B    Altcode:
  We determine the plasma physical parameters of an erupting prominence
  embedded in the core of a CME, combininging visible light coronagraphic
  images from SOHO/LASCO with UV spectra acquired by SOHO/UVCS. Strong
  UV emissions were detected in the hydrogen Lyman-α and Lyman-β
  lines and C III line. Visible light and UV intensities have been used
  to estimate the projected thickness and velocity of the prominence,
  together with the effective plasma temperature, microturbolent velocity,
  and column density. These parameters have been used to constrain
  1D NLTE modeling of the erupting plasma, taking into account the
  effects of large flow velocities (Doppler dimming). Roughly one-half
  of considered points in the prominence body show a non-negligible
  Lyman-α optical thickness. Comparison between the calculated and the
  measured intensities of the two Lyman lines was also used to derive the
  geometrical filling factor. Results show that the erupting prominence
  plasma is relatively hot, with a low electron density, a wide range of
  effective thicknesses, a rather narrow range of radial flow velocities,
  and a microturbulence of about 25 km/s. This analysis provides a basis
  for future diagnostics of prominences using the METIS coronagraph on
  board the Solar Orbiter mission.

---------------------------------------------------------
Title: Dynamics in quiescent prominences observed by the IRIS and
    MSDP spectrographs
Authors: Gunár, Stanislav; Schmieder, Brigitte; Ruan, Guiping; Mein,
   Pierre; Heinzel, Petr
2018cosp...42E1314G    Altcode:
  Quiescent solar prominences are generally considered to
  be stable. However, these prominences consist of a multitude of
  small-scale structures or threads that are often significantly
  dynamic. To understand the nature of the plasma dynamics we use the
  high spatial, temporal and spectral resolution observations obtained
  by IRIS during coordinated campaign with the MSDP spectrograph
  at the Meudon Solar Tower. Mg II h and k lines observed by IRIS
  represent a good diagnostic tool for investigation of the prominence
  fine structure dynamics, as they are optically thick under the
  prominence conditions. We will present detailed IRIS observations of
  Mg II lines. We explain significant asymmetries in the observed Mg II
  spectra by the presence of several threads located along the line of
  sight with different velocities. In such a case, the decrease of the
  intensity of individual components of the observed spectra with the
  distance from the central wavelength can be explained by the Doppler
  dimming effect. To interpret the observed Mg II profiles in terms
  of dynamics we use 1D or 2D radiative transfer models including a
  prominence-corona transition region. We also show that the H-alpha
  line which is optically thinner than the Mg II doublet is an important
  constrain for the radiative transfer radiation modelling.

---------------------------------------------------------
Title: Hot Erupting Prominences in Cores of Cme's
Authors: Heinzel, Petr; Bemporad, Alessandro; Anzer, Ulrich; Jejcic,
   Sonja; Susino, Roberto; Dzifcakova, Elena
2018cosp...42E1421H    Altcode:
  Coronal mass ejections (CME) associated with prominence eruptions
  exhibit relatively coolmaterial in their cores. Such prominence
  plasmas were frequently detected in various spectrallines by SOHO/UVCS
  coronagraph and in the visible light by SOHO/LASCO as well as bySTEREO
  coronagraphs. UVCS provided excellent spectra of CME-core prominences
  and anextended catalogue of these data is available. We will present
  recent results of a hot prominence diagnostics using the hydrogen Lyman
  lines and the CIII line . The erupting prominence parameters are further
  constrained by the visible light observations from LASCO-C2. A novel
  non-LTE modeling based on such observations will be presented and we
  will highlight the diagnostic potential of the UV and visible light for
  future space coronagraphs like Metis on board the ESA Solar Orbiter
  mission. The plasma parameters of such hot prominences are compared
  with those obtained from numerical MHD simulations of erupting flux
  ropes surrounded by CMEs. Finally, we will also mention synergies with
  stellar analogues.

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Title: Can 3D whole-prominence fine structure models be used for
    assessment of the prominence plasma mass and distribution prior to
    the onset of CMEs?
Authors: Gunár, Stanislav; Schmieder, Brigitte; Aulanier, Guillaume;
   Anzer, Ulrich; Heinzel, Petr; Mackay, Duncan; Dudik, Jaroslav
2018cosp...42E1316G    Altcode:
  Two complex 3D models of entire prominences including their numerous
  fine structures were recently developed. The first 3D Whole-Prominence
  Fine Structure (WPFS) model was developed by Gunár and Mackay. The
  second 3D WPFS model was put forward by Gunár, Aulanier, Dudík,
  Heinzel, and Schmieder. These 3D prominence models combine simulations
  of the 3D magnetic field configuration of an entire prominence with a
  detailed description of the prominence plasma. The plasma is located
  in magnetic dips in hydrostatic equilibrium and is distributed
  along hundreds of fine structures. The assumed prominence plasma
  has realistic density and temperature distributions including the
  prominence-corona transition region.These 3D WPFS models allow us
  to study the distribution and the mass of the prominence plasma
  contained in prominence magnetic field configurations. These can
  be crucial during the onset and early evolution of CMEs. Moreover,
  prominence plasma represents a bulk of the material ejected by CMEs
  into the interplanetary space. Here, we investigate the potential of
  using the 3D WPFS models for assessment of the role the prominence
  plasma plays in the initiation and evolution of CMEs.

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Title: IRIS Observations and Modeling of MGII Flare Loops
Authors: Heinzel, Petr; Berlicki, Arkadiusz; Mikula, Katarzyna;
   Liu, Wenjuan
2018cosp...42E1423H    Altcode:
  Solar chromospheric flares are often associated with cool loops which
  are rooted in the ribbons. These loops extend into coronal altitudes
  and usually are modelled as prominence-like structures illuminated from
  the solar disk. The loops exhibit large down-flows (coronal rain) and
  they evolve in time in accordance with the characteristic cooling times
  of the loop plasmas. Cool loops are visible in various spectral lines
  formed at chromospheric temperatures. We exploit novel observations
  of such loops in MgII h and k lines obtained by the IRIS satellite,
  analyse selected observations where the cool loops are well visible
  and studytheir temporal evolution. Our spectroscopic diagnostics is
  based on 2D non-LTE modelling ofMgII lines in flare loops taking into
  account the flows along the loops. From these models wedetermine various
  plasma parameters and the rates of radiation cooling. These results
  allow usto better understand the structure, dynamics and evolution of
  cool flare loops.

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Title: Blue wing enhancement of the chromospheric Mg II h and k
    lines in a solar flare
Authors: Tei, Akiko; Shibata, Kazunari; Asai, Ayumi; Ichimoto,
   Kiyoshi; Heinzel, Petr; Ueno, Satoru; Okamoto, Joten; Sakaue, Takahito;
   Kawate, Tomoko
2018cosp...42E3350T    Altcode:
  We performed coordinated observations of NOAA AR 12205, which produced
  a C-class flare on 2014 November 11, with the Interface Region Imaging
  Spectrograph (IRIS) and the Domeless Solar Telescope (DST) at Hida
  Observatory.Using spectral data in the Si IV 1403 Å, C II 1335 Å,
  and Mg II h and k lines from IRIS and the Ca II K, Ca II 8542 Å,
  and Hα lines from DST, we investigated the temporal and spatial
  evolution around a moving flare kernel.In the Mg II h line, the leading
  edge of the kernel showed intensity enhancement in the blue wing and
  difference between the blue-side peak and red-side one (I_{h2v} &lt;
  I_{h2r}).Then, the drastic change of the intensity in the red wing
  occurred.The blueshift lasted for 9-48 s with a speed of 10.1 ± 2.6
  km s^{-1} and it was followed by the strong redshift with a speed of
  up to 51 km s^{-1} detected in the Mg II h line.The strong redshift
  was a common property for all six lines but the blueshift prior to it
  was found only in the Mg II lines.A cloud modeling of the Mg II h line
  suggests that the blue wing enhancement with such peak difference can
  be caused by a chromospheric-temperature (cool) upflow.We discuss a
  scenario in which an upflow of cool plasma is lifted up by expanding
  (hot) plasma owing to the deep penetration of non-thermal electrons
  into the chromosphere.In addition, at the leading edge of the final
  flare footpoints, the blueshift persisted in the Mg II h line, which
  was not followed by any large redshift and intensity enhancement.Such
  long-lasting blueshift can be explained by cool upflow caused by small
  energy flux into the lower atmosphere.

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Title: Cool Loops on Cool Stars
Authors: Heinzel, Petr
2018cosp...42E1422H    Altcode:
  Recently a significant effort has been devoted to systematic modelling
  of solar and stellar chromospheric flares which are typically manifested
  by bright ribbons embedded in the lower atmospheric layers. However,
  apart from ribbons detectable in a broad range of the electromagnetic
  spectrum, overlying loops are also frequently observed on the Sun. They
  appear in various spectral lines and can be well resolved in the
  so-called eruptive flares. We will show how their appearance depends
  on the loop plasma conditions and parameters. We will also briefly
  review the efforts to model the radiation properties of such loops and
  namely of those which cooled down to chromospheric temperatures. Light
  curves of the flaring ribbons may differ from time evolution of the
  loop brightness and this can be easily detected on the Sun. However,
  on cool stars the measured light curves may contain an unresolved
  information about the temporal evolution of both ribbons and cool
  loops and we will demonstrate how this can be modelled.

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Title: Can Flare Loops Contribute to the White-light Emission of
    Stellar Superflares?
Authors: Heinzel, P.; Shibata, K.
2018ApJ...859..143H    Altcode: 2018arXiv180409656H
  Since the discovery of stellar superflares by the Kepler satellite,
  these extremely energetic events have been studied in analogy to
  solar flares. Their white-light (WL) continuum emission has been
  interpreted as being produced by heated ribbons. In this paper,
  we compute the WL emission from overlying flare loops depending
  on their density and temperature and show that, under conditions
  expected during superflares, the continuum brightening due to
  extended loop arcades can significantly contribute to stellar flux
  detected by Kepler. This requires electron densities in the loops of
  10<SUP>12</SUP>-10<SUP>13</SUP> cm<SUP>-3</SUP> or higher. We show
  that such densities, exceeding those typically present in solar-flare
  loops, can be reached on M-dwarf and solar-type superflare stars with
  large starspots and much stronger magnetic fields. Quite importantly,
  the WL radiation of loops is not very sensitive to their temperature
  and thus both cool as well as hot loops may contribute. We show that
  the WL intensity emergent from optically thin loops is lower than the
  blackbody radiation from flare ribbons, but the contribution of loops
  to total stellar flux can be quite important due to their significant
  emitting areas. This new scenario for interpreting superflare emission
  suggests that the observed WL flux is due to a mixture of the ribbon
  and loop radiation and can be even loop-dominated during the gradual
  phase of superflares.

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Title: Observation of the X9.3 flare of September 6 2017 in UV/EUV
    by PROBA2/LYRA
Authors: Dominique, Marie; Zhukov, Andrei; Heinzel, Petr; Dammasch,
   Ingolf E.; Wauters, Laurence; Dolla, Laurent; Shestov, Sergei
2018tess.conf31903D    Altcode:
  After several months of relative quietness, a sudden burst of solar
  activity was observed starting on September 4 2017, when the NOAA AR
  12673 started to develop quickly. This region remained active until it
  disappeared behind the west limb on September 10. It produced multiple
  strong flares (27 M-class flares and 4 X-class flares). Among them,
  there were the two strongest flare observed so far during the solar
  cycle 24: the X9.3 flare of September 6 and the off-limb X8.3 flare of
  September 10. <P />At the time of these two events, the Large-Yield
  Radiometer (LYRA) onboard PROBA2 was performing a special flare
  observation campaign, involving one of its spare units that is normally
  only used for calibration purposes. As this unit was only sporadically
  opened over the mission lifetime, it is relatively preserved from the
  ageing processes that otherwise affect the instrument, and it delivered
  very clear observations of both flares. In particular, the X9.3 flare
  produced a signature in the four channels of the instrument, of which
  two observe the EUV range, one the hydrogen Lyman-alpha line, and the
  last one the continuum around 2000 Angstroms. As flare observations
  are relatively rare in Lyman-alpha and almost non-existing in the
  continuum around 2000 Angstroms, this constitutes a rather unique set
  of observations. In contrast, the X8.3 flare only produced signatures
  in the two EUV channels. <P />This presentation will describe the
  LYRA observations, compare both flares, and discuss the origin of the
  emitted signal in the four channels.

---------------------------------------------------------
Title: Václav Bumba (1925 - 2018)
Authors: Kotrč, Pavel; Heinzel, Petr; Sobotka, Michal; Ambrož,
   Pavel; van Driel-Gesztelyi, Lidia
2018SoPh..293...40K    Altcode:
  No abstract at ADS

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Title: Visibility of Prominences Using the He I D<SUB>3</SUB> Line
    Filter on the PROBA-3/ASPIICS Coronagraph
Authors: Jejčič, S.; Heinzel, P.; Labrosse, N.; Zhukov, A. N.;
   Bemporad, A.; Fineschi, S.; Gunár, S.
2018SoPh..293...33J    Altcode: 2018arXiv180700155J
  We determine the optimal width and shape of the narrow-band filter
  centered on the He I D<SUB>3</SUB> line for prominence and coronal
  mass ejection (CME) observations with the ASPIICS (Association of
  Spacecraft for Polarimetric and Imaging Investigation of the Corona of
  the Sun) coronagraph onboard the PROBA-3 (Project for On-board Autonomy)
  satellite, to be launched in 2020. We analyze He I D<SUB>3</SUB> line
  intensities for three representative non-local thermal equilibrium
  prominence models at temperatures 8, 30, and 100 kK computed with a
  radiative transfer code and the prominence visible-light (VL) emission
  due to Thomson scattering on the prominence electrons. We compute
  various useful relations at prominence line-of-sight velocities of 0,
  100, and 300 km s<SUP>−1</SUP> for 20 Å wide flat filter and three
  Gaussian filters with a full-width at half-maximum (FWHM) equal to 5,
  10, and 20 Å to show the relative brightness contribution of the He I
  D<SUB>3</SUB> line and the prominence VL to the visibility in a given
  narrow-band filter. We also discuss possible signal contamination by Na
  I D<SUB>1</SUB> and D<SUB>2</SUB> lines, which otherwise may be useful
  to detect comets. Our results mainly show that i) an optimal narrow-band
  filter should be flat or somewhere between flat and Gaussian with an
  FWHM of 20 Å in order to detect fast-moving prominence structures,
  ii) the maximum emission in the He I D<SUB>3</SUB> line is at 30 kK
  and the minimal at 100 kK, and iii) the ratio of emission in the He I
  D<SUB>3</SUB> line to the VL emission can provide a useful diagnostic
  for the temperature of prominence structures. This ratio is up to 10
  for hot prominence structures, up to 100 for cool structures, and up
  to 1000 for warm structures.

---------------------------------------------------------
Title: Quiescent Prominences in the Era of ALMA. II. Kinetic
    Temperature Diagnostics
Authors: Gunár, Stanislav; Heinzel, Petr; Anzer, Ulrich; Mackay,
   Duncan H.
2018ApJ...853...21G    Altcode:
  We provide the theoretical background for diagnostics of the thermal
  properties of solar prominences observed by the Atacama Large
  Millimeter/submillimeter Array (ALMA). To do this, we employ the 3D
  Whole-Prominence Fine Structure (WPFS) model that produces synthetic
  ALMA-like observations of a complex simulated prominence. We use
  synthetic observations derived at two different submillimeter/millimeter
  (SMM) wavelengths—one at a wavelength at which the simulated
  prominence is completely optically thin and another at a wavelength at
  which a significant portion of the simulated prominence is optically
  thick—as if these were the actual ALMA observations. This allows
  us to develop a technique for an analysis of the prominence plasma
  thermal properties from such a pair of simultaneous high-resolution ALMA
  observations. The 3D WPFS model also provides detailed information about
  the distribution of the kinetic temperature and the optical thickness
  along any line of sight. We can thus assess whether the measure of the
  kinetic temperature derived from observations accurately represents
  the actual kinetic temperature properties of the observed plasma. We
  demonstrate here that in a given pixel the optical thickness at the
  wavelength at which the prominence plasma is optically thick needs
  to be above unity or even larger to achieve a sufficient accuracy of
  the derived information about the kinetic temperature of the analyzed
  plasma. Information about the optical thickness cannot be directly
  discerned from observations at the SMM wavelengths alone. However,
  we show that a criterion that can identify those pixels in which
  the derived kinetic temperature values correspond well to the actual
  thermal properties in which the observed prominence can be established.

---------------------------------------------------------
Title: ASPIICS: a giant, white light and emission line coronagraph
    for the ESA proba-3 formation flight mission
Authors: Lamy, P. L.; Vivès, S.; Curdt, W.; Damé, L.; Davila, J.;
   Defise, J. -M.; Fineschi, S.; Heinzel, P.; Howard, Russel; Kuzin,
   S.; Schmutz, W.; Tsinganos, K.; Zhukov, A.
2017SPIE10565E..0TL    Altcode:
  Classical externally-occulted coronagraphs are presently limited in
  their performances by the distance between the external occulter and
  the front objective. The diffraction fringe from the occulter and
  the vignetted pupil which degrades the spatial resolution prevent
  useful observations of the white light corona inside typically 2-2.5
  solar radii (Rsun). Formation flying offers and elegant solution to
  these limitations and allows conceiving giant, externally-occulted
  coronagraphs using a two-component space system with the external
  occulter on one spacecraft and the optical instrument on the
  other spacecraft at a distance of hundred meters [1, 2]. Such
  an instrument ASPIICS (Association de Satellites Pour l'Imagerie
  et l'Interférométrie de la Couronne Solaire) has been selected
  by the European Space Agency (ESA) to fly on its PROBA-3 mission
  of formation flying demonstration which is presently in phase B
  (Fig. 1). The classical design of an externally-occulted coronagraph is
  adapted to the formation flying configuration allowing the detection
  of the very inner corona as close as 0.04 solar radii from the solar
  limb. By tuning the position of the occulter spacecraft, it may even be
  possible to reach the chromosphere and the upper part of the spicules
  [3]. ASPIICS will perform (i) high spatial resolution imaging of the
  continuum K+F corona in photometric and polarimetric modes, (ii) high
  spatial resolution imaging of the E-corona in two coronal emission lines
  (CEL): Fe XIV and He I D3, and (iii) two-dimensional spectrophotometry
  of the Fe XIV emission line. ASPIICS will address the question of the
  coronal heating and the role of waves by characterizing propagating
  fluctuations (waves and turbulence) in the solar wind acceleration
  region and by looking for oscillations in the intensity and Doppler
  shift of spectral lines. The combined imaging and spectral diagnostics
  capabilities available with ASPIICS will allow mapping the velocity
  field of the corona both in the sky plane (directly on the images)
  and along the line-of-sight by measuring the Doppler shifts of
  emission lines in an effort to determine how the different components
  of the solar wind, slow and fast are accelerated. With a possible
  launch in 2014, ASPIICS will observe the corona during the maximum of
  solar activity, insuring the detection of many Coronal Mass Ejections
  (CMEs). By rapidly alternating high-resolution imaging and spectroscopy,
  CMEs will be thoroughly characterized.

---------------------------------------------------------
Title: Hot prominence detected in the core of a coronal mass
    ejection. II. Analysis of the C III line detected by SOHO/UVCS
Authors: Jejčič, S.; Susino, R.; Heinzel, P.; Dzifčáková, E.;
   Bemporad, A.; Anzer, U.
2017A&A...607A..80J    Altcode:
  Context. We study the physics of erupting prominences in the core
  of coronal mass ejections (CMEs) and present a continuation of a
  previous analysis. <BR /> Aims: We determine the kinetic temperature
  and microturbulent velocity of an erupting prominence embedded in the
  core of a CME that occurred on August 2, 2000 using the Ultraviolet
  Coronagraph and Spectrometer observations (UVCS) on board the Solar
  and Heliospheric Observatory (SOHO) simultaneously in the hydrogen
  Lα and C III lines. We develop the non-LTE (departures from the local
  thermodynamic equilibrium - LTE) spectral diagnostics based on Lα and
  Lβ measured integrated intensities to derive other physical quantities
  of the hot erupting prominence. Based on this, we synthesize the C
  III line intensity to compare it with observations. <BR /> Methods:
  Our method is based on non-LTE modeling of eruptive prominences. We
  used a general non-LTE radiative-transfer code only for optically thin
  prominence points because optically thick points do not allow the
  direct determination of the kinetic temperature and microturbulence
  from the line profiles. The input parameters of the code were the
  kinetic temperature and microturbulent velocity derived from the Lα
  and C III line widths, as well as the integrated intensity of the Lα
  and Lβ lines. The code runs in three loops to compute the radial flow
  velocity, electron density, and effective thickness as the best fit
  to the Lα and Lβ integrated intensities within the accuracy defined
  by the absolute radiometric calibration of UVCS data. <BR /> Results:
  We analyzed 39 observational points along the whole erupting prominence
  because for these points we found a solution for the kinetic temperature
  and microturbulent velocity. For these points we ran the non-LTE code to
  determine best-fit models. All models with τ<SUB>0</SUB>(Lα) ≤ 0.3
  and τ<SUB>0</SUB>(C III) ≤ 0.3 were analyzed further, for which we
  computed the integrated intensity of the C III line using a two-level
  atom. The best agreement between computed and observed integrated
  intensity led to 30 optically thin points along the prominence. The
  results are presented as histograms of the kinetic temperature,
  microturbulent velocity, effective thickness, radial flow velocity,
  electron density, and gas pressure. We also show the relation between
  the microturbulence and kinetic temperature together with a scatter plot
  of computed versus observed C III integrated intensities and the ratio
  of the computed to observed C III integrated intensities versus kinetic
  temperature. <BR /> Conclusions: The erupting prominence embedded in
  the CME is relatively hot with a low electron density, a wide range of
  effective thicknesses, a rather narrow range of radial flow velocities,
  and a microturbulence of about 25 km s<SUP>-1</SUP>. This analysis shows
  a disagreement between observed and synthetic intensities of the C III
  line, the reason for which most probably is that photoionization is
  neglected in calculations of the ionization equilibrium. Alternatively,
  the disagreement might be due to non-equilibrium processes.

---------------------------------------------------------
Title: On the Nature of Off-limb Flare Continuum Sources Detected
    by SDO/HMI
Authors: Heinzel, P.; Kleint, L.; Kašparová, J.; Krucker, S.
2017ApJ...847...48H    Altcode: 2017arXiv170906377H
  The Helioseismic and Magnetic Imager on board the Solar Dynamics
  Observatory has provided unique observations of off-limb flare
  emission. White-light continuum enhancements were detected in the
  “continuum” channel of the Fe 6173 Å line during the impulsive
  phase of the observed flares. In this paper we aim to determine which
  radiation mechanism is responsible for such enhancement being seen above
  the limb, at chromospheric heights around or below 1000 km. Using a
  simple analytical approach, we compare two candidate mechanisms, the
  hydrogen recombination continuum (Paschen) and the Thomson continuum
  due to scattering of disk radiation on flare electrons. Both mechanisms
  depend on the electron density, which is typically enhanced during the
  impulsive phase of a flare as the result of collisional ionization (both
  thermal and also non-thermal due to electron beams). We conclude that
  for electron densities higher than 10<SUP>12</SUP> cm<SUP>-3</SUP>,
  the Paschen recombination continuum significantly dominates the
  Thomson scattering continuum and there is some contribution from the
  hydrogen free-free emission. This is further supported by detailed
  radiation-hydrodynamical (RHD) simulations of the flare chromosphere
  heated by the electron beams. We use the RHD code FLARIX to compute the
  temporal evolution of the flare-heating in a semi-circular loop. The
  synthesized continuum structure above the limb resembles the off-limb
  flare structures detected by HMI, namely their height above the limb,
  as well as the radiation intensity. These results are consistent with
  recent findings related to hydrogen Balmer continuum enhancements,
  which were clearly detected in disk flares by the IRIS near-ultraviolet
  spectrometer.

---------------------------------------------------------
Title: Structure and Dynamics of Cool Flare Loops Observed by the
    Interface Region Imaging Spectrograph
Authors: Mikuła, K.; Heinzel, P.; Liu, W.; Berlicki, A.
2017ApJ...845...30M    Altcode:
  Flare loops were well observed with the Interface Region Imaging
  Spectrograph (IRIS) during the gradual phase of two solar flares
  on 2014 March 29 and 2015 June 22. Cool flare loops are visible in
  various spectral lines formed at chromospheric and transition-region
  temperatures and exhibit large downflows which correspond to the
  standard scenario. The principal aim of this work is to analyze
  the structure and dynamics of cool flare loops observed in Mg II
  lines. Synthetic profiles of the Mg II h line are computed using the
  classical cloud model and assuming a uniform background intensity. In
  this paper, we study novel IRIS NUV observations of such loops in Mg II
  h and k lines and also show the behavior of hotter lines detected in
  the FUV channel. We obtained the spatial evolution of the velocities:
  near the loop top, the flow velocities are small and they are increasing
  toward the loop legs. Moreover, from slit-jaw image (SJI) movies, we
  observe some plasma upflows into the loops, which are also detectable
  in Mg II spectra. The brightness of the loops systematically decreases
  with increasing flow velocity, and we ascribe this to the effect of
  Doppler dimming, which works for Mg II lines. Emission profiles of Mg
  II were found to be extremely broad, and we explain this through the
  large unresolved non-thermal motions.

---------------------------------------------------------
Title: On the Origin of the Flare Emission in IRIS’ SJI 2832
Filter:Balmer Continuum or Spectral Lines?
Authors: Kleint, Lucia; Heinzel, Petr; Krucker, Säm
2017ApJ...837..160K    Altcode: 2017arXiv170207167K
  Continuum (“white-light,” WL) emission dominates the energetics of
  flares. Filter-based observations, such as the IRIS SJI 2832 filter,
  show WL-like brightenings during flares, but it is unclear whether
  the emission arises from real continuum emission or enhanced spectral
  lines, possibly turning into emission. The difficulty in filter-based
  observations, contrary to spectral observations, is to determine which
  processes contribute to the observed brightening during flares. Here
  we determine the contribution of the Balmer continuum and the spectral
  line emission to IRIS’ SJI 2832 emission by analyzing the appropriate
  passband in simultaneous IRIS NUV spectra. We find that spectral line
  emission can contribute up to 100% to the observed slitjaw images (SJI)
  emission, that the relative contributions usually temporally vary,
  and that the highest SJI enhancements that are observed are most likely
  because of the Balmer continuum. We conclude that care should be taken
  when calling SJI 2832 a continuum filter during flares, because the
  influence of the lines on the emission can be significant.

---------------------------------------------------------
Title: Extreme Space Weather in Extra-Solar Systems - a Flare
    Alert Program
Authors: Hanslmeier, A.; Leitzinger, M.; Greimel, R.; Odert, P.;
   Ratzka, T.; Brajša, R.; Guenther, E. W.; Korhonen, H.; Pribulla, T.;
   Šlechta, M.; Vida, K.; Güdel, M.; Heinzel, P.; Lammer, H.; Ribas, I.
2017CEAB...41...67H    Altcode:
  Highly energetic stellar activity phenomena, such as outbreaks of
  radiations (flares) and mass expulsions into the helio-/astro-sphere
  (coronal mass ejections/CMEs), may have a severe impact on
  the atmospheric evolution of planets. Stellar flare have been
  studied for decades now and their typical parameters are determined
  statistically. However, observations of stellar CMEs are rare, yielding
  only a handful of detections so far. The detection of CMEs on stars
  demands more observational effort than the detection flares, because
  the circumstellar environment cannot be spatially resolved like in the
  Solar System. The most convincing detections up to now were found as
  Doppler-shifted Balmer line extra-emission/absorption features emerging
  close to flare events, indicating the rise end ejection of prominence
  material embedded in the CME core. Dedicated programs aiming for a
  statistical determination of occurrence rates and the parameters of
  stellar CMEs are still lacking. Therefore, we propose an innovative
  and efficient observational approach to search for and characterize
  CMEs on Sun-like and late-type pre-main sequence and main sequence
  stars to determine stellar CME parameters and their occurrence rates
  as a function of stellar spectral type and age, as well as establish
  a stellar flare/CME association rate, for the first time ever.

---------------------------------------------------------
Title: Quiescent Prominences in the Era of ALMA: Simulated
    Observations Using the 3D Whole-prominence Fine Structure Model
Authors: Gunár, Stanislav; Heinzel, Petr; Mackay, Duncan H.; Anzer,
   Ulrich
2016ApJ...833..141G    Altcode:
  We use the detailed 3D whole-prominence fine structure model to
  produce the first simulated high-resolution ALMA observations
  of a modeled quiescent solar prominence. The maps of synthetic
  brightness temperature and optical thickness shown in the present
  paper are produced using a visualization method for synthesis of the
  submillimeter/millimeter radio continua. We have obtained the simulated
  observations of both the prominence at the limb and the filament
  on the disk at wavelengths covering a broad range that encompasses
  the full potential of ALMA. We demonstrate here extent to which the
  small-scale and large-scale prominence and filament structures will be
  visible in the ALMA observations spanning both the optically thin and
  thick regimes. We analyze the relationship between the brightness and
  kinetic temperature of the prominence plasma. We also illustrate the
  opportunities ALMA will provide for studying the thermal structure
  of the prominence plasma from the cores of the cool prominence fine
  structure to the prominence-corona transition region. In addition, we
  show that detailed 3D modeling of entire prominences with their numerous
  fine structures will be important for the correct interpretation of
  future ALMA observations of prominences.

---------------------------------------------------------
Title: NLTE modeling of a small active region filament observed with
    the VTT
Authors: Schwartz, P.; Balthasar, H.; Kuckein, C.; Koza, J.; Gömöry,
   P.; Rybák, J.; Heinzel, P.; Kučera, A.
2016AN....337.1045S    Altcode:
  An active region mini-discretionary-filament was observed with the
  Vacuum Tower Telescope (VTT) in Tenerife simultaneously in the He
  I infrared triplet using the Tenerife Infrared Polarimeter 1 (TIP
  1), in Hα with the TESOS Fabry-Pérot interferometer, and in Ca II
  8542 Å with the VTT spectrograph. The spectropolarimetric data were
  inverted using the HAZEL code and Hα profiles were modelled by solving
  a NLTE radiative transfer in a simple isobaric and isothermal 2D slab
  irradiated both from its bottom and sides from the solar surface. It was
  found that the mini-discretionary-filament is composed of horizontal
  fluxtubes, along which the cool plasma of T∼10 000 K can flow with
  very large, even supersonic, velocities.

---------------------------------------------------------
Title: On measurements of the Balmer continuum flux in a solar flare:
    Analysis of pre-flare and flare pulsations
Authors: Zapiór, M.; Kotrč, P.; Oliver, R.; Procházka, O.;
   Heinzel, P.
2016AN....337.1078Z    Altcode:
  A new ground based device for the measurement of the Balmer continuum
  flux in solar flares was recently developed and installed at the
  Ondřejov Observatory. We observed an X1 solar flare on 2014 June 11
  during its pre-flare and impulsive phases using a wide band spectrometer
  with a cadence of 1 s. The Ensemble Empirical Mode Decomposition (EEMD)
  of the registered signal was performed. We found damped oscillations
  with a period of 609 s and damping time of 1478 s. Shorter periods of
  about 30-120 s were found during the pre-flare and impulsive phases,
  but they might be of non-flare origin.

---------------------------------------------------------
Title: Height formation of bright points observed by IRIS in Mg II
    line wings during flux emergence
Authors: Grubecka, M.; Schmieder, B.; Berlicki, A.; Heinzel, P.;
   Dalmasse, K.; Mein, P.
2016A&A...593A..32G    Altcode:
  Context. A flux emergence in the active region AR 111850 was observed
  on September 24, 2013 with the Interface Region Imaging Spectrograph
  (IRIS). Many bright points are associated with the new emerging flux
  and show enhancement brightening in the UV spectra. <BR /> Aims:
  The aim of this work is to compute the altitude formation of the
  compact bright points (CBs) observed in Mg II lines in the context
  of searching Ellerman bombs (EBs). <BR /> Methods: IRIS provided two
  large dense rasters of spectra in Mg II h and k lines, Mg II triplet,
  C II and Si IV lines covering all the active region and slit jaws in
  the two bandpasses (1400 Å and 2796 Å) starting at 11:44 UT and
  15:39 UT, and lasting 20 min each. Synthetic profiles of Mg II and
  Hα lines are computed with non-local thermodynamic equlibrium (NLTE)
  radiative transfer treatment in 1D solar atmosphere model including
  a hotspot region defined by three parameters: temperature, altitude,
  and width. <BR /> Results: Within the two IRIS rasters, 74 CBs are
  detected in the far wings of the Mg II lines (at +/-1 Å and 3.5
  Å). Around 10% of CBs have a signature in Si IV and CII. NLTE models
  with a hotspot located in the low atmosphere were found to fit a sample
  of Mg II profiles in CBs. The Hα profiles computed with these Mg II
  CB models are consistent with typical EB profiles observed from ground
  based telescopes e.g. THEMIS. A 2D NLTE modelling of fibrils (canopy)
  demonstrates that the Mg II line centres can be significantly affected
  but not the peaks and the wings of Mg II lines. <BR /> Conclusions:
  We conclude that the bright points observed in Mg II lines can be
  formed in an extended domain of altitudes in the photosphere and/or
  the chromosphere (400 to 750 km). Our results are consistent with the
  theory of heating by Joule dissipation in the atmosphere produced by
  magnetic field reconnection during flux emergence.

---------------------------------------------------------
Title: Synthetic Hydrogen Spectra of Oscillating Prominence Slabs
    Immersed in the Solar Corona
Authors: Zapiór, M.; Oliver, R.; Ballester, J. L.; Heinzel, P.
2016ApJ...827..131Z    Altcode:
  We study the behavior of Hα and Hβ spectral lines and their spectral
  indicators in an oscillating solar prominence slab surrounded by the
  solar corona, using an MHD model combined with a 1D radiative transfer
  code taken in the line of sight perpendicular to the slab. We calculate
  the time variation of the Doppler shift, half-width, and maximum
  intensity of the Hα and Hβ spectral lines for different modes of
  oscillation. We find a non-sinusoidal time dependence of some spectral
  parameters with time. Because Hα and Hβ spectral indicators have
  different behavior for different modes, caused by differing optical
  depths of formation and different plasma parameter variations in
  time and along the slab, they may be used for prominence seismology,
  especially to derive the internal velocity field in prominences.

---------------------------------------------------------
Title: Flares In Time-Domain Surveys
Authors: Kowalski, Adam; Hawley, Suzanne; Davenport, James; Berlicki,
   Arkadiusz; Cauzzi, Gianna; Fletcher, Lyndsay; Heinzel, Petr; Notsu,
   Yuta; Loyd, Parke; Martinez Oliveros, Juan Carlos; Pugh, Chloe;
   Schmidt, Sarah Jane; Karmakar, Subhajeet; Pye, John; Flaccomio, Ettore
2016csss.confE.126K    Altcode:
  Proceedings for the splinter session "Flares in Time-Domain Surveys"
  convened at Cool Stars 19 on June 07, 2016 in Uppsala, Sweden. Contains
  a two page summary of the splinter session, links to YouTube talks,
  and a PDF copy of the slides from the presenters.

---------------------------------------------------------
Title: Chromospheric Heating by Acoustic Waves Compared to Radiative
    Cooling
Authors: Sobotka, M.; Heinzel, P.; Švanda, M.; Jurčák, J.; del Moro,
   D.; Berrilli, F.
2016ApJ...826...49S    Altcode: 2016arXiv160504794S
  Acoustic and magnetoacoustic waves are among the possible candidate
  mechanisms that heat the upper layers of the solar atmosphere. A weak
  chromospheric plage near the large solar pore NOAA 11005 was observed
  on 2008 October 15, in the Fe I 617.3 nm and Ca II 853.2 nm lines of
  the Interferometric Bidimemsional Spectrometer attached to the Dunn
  Solar Telescope. In analyzing the Ca II observations (with spatial
  and temporal resolutions of 0.″4 and 52 s) the energy deposited by
  acoustic waves is compared to that released by radiative losses. The
  deposited acoustic flux is estimated from the power spectra of Doppler
  oscillations measured in the Ca II line core. The radiative losses
  are calculated using a grid of seven one-dimensional hydrostatic
  semi-empirical model atmospheres. The comparison shows that the
  spatial correlation of the maps of radiative losses and acoustic flux
  is 72%. In a quiet chromosphere, the contribution of acoustic energy
  flux to radiative losses is small, only about 15%. In active areas
  with a photospheric magnetic-field strength between 300 and 1300 G
  and an inclination of 20°-60°, the contribution increases from 23%
  (chromospheric network) to 54% (a plage). However, these values have
  to be considered as lower limits and it might be possible that the
  acoustic energy flux is the main contributor to the heating of bright
  chromospheric network and plages.

---------------------------------------------------------
Title: Hot prominence detected in the core of a coronal mass ejection:
    Analysis of SOHO/UVCS Lα and SOHO/LASCO visible-light observations
Authors: Heinzel, P.; Susino, R.; Jejčič, S.; Bemporad, A.; Anzer, U.
2016A&A...589A.128H    Altcode:
  Context. The paper deals with the physics of erupting prominences in
  the core of coronal mass ejections (CME). <BR /> Aims: We determine the
  physical parameters of an erupting prominence embedded in the core of a
  CME using SOHO/UVCS hydrogen Lα and Lβ lines and SOHO/LASCO visible
  light observations. In particular we analyze the CME event observed
  on August 2, 2000. We develop the non-LTE (NLTE; I.e. considering
  departures from the local thermodynamic equilibrium - LTE) spectral
  diagnostics based on Lα and visible light observations. <BR /> Methods:
  Our method is based on 1D NLTE modeling of eruptive prominences and
  takes into account the effect of large flow velocities, which reach
  up to 300 km s<SUP>-1</SUP> for the studied event (the so-called
  Doppler dimming). The NLTE radiative-transfer method can be used
  for both optically thin and thick prominence structures. We combine
  spectroscopic UVCS observations of an erupting prominence in the core
  of a CME with visible light images from LASCO-C2 in order to derive the
  geometrical parameters like projected thickness and velocity, together
  with the effective temperature and column density of electrons. These
  are then used to constrain our NLTE radiative transfer modeling which
  provides the kinetic temperature, microturbulent velocity, gas pressure,
  ionization degree, the line opacities, and the prominence effective
  thickness (geometrical filling factor). <BR /> Results: Analysis was
  made for 69 observational points (spatial pixels) inside the whole
  erupting prominence. Roughly one-half of them show a non-negligible Lα
  optical thickness for flow velocity 300 km s<SUP>-1</SUP> and about
  one-third for flow velocity 150 km s<SUP>-1</SUP>. All pixels with
  Lατ<SUB>0</SUB> ≤ 0.3 have been considered for further analysis,
  which is presented in the form of statistical distributions (histograms)
  of various physical quantities such as the kinetic temperature, gas
  pressure, and electron density for two representative flow velocities
  (150 and 300 km s<SUP>-1</SUP>) and non-zero microturbulence. For
  two pixels co-temporal LASCO visible-light data are also available,
  which further constrains the diagnostics of the electron density and
  effective thickness. Detailed NLTE modeling is presented for various
  sets of input parameters. <BR /> Conclusions: The studied CME event
  shows that the erupting prominence expands to large volumes, meaning
  that it is a low-pressure structure with low electron densities and
  high temperatures. This analysis provides a basis for future diagnostics
  using the METIS coronagraph on board the Solar Orbiter mission.

---------------------------------------------------------
Title: The dynamics and magnetism of the X1 flare on 2014-03-29
Authors: Kleint, Lucia; Heinzel, Petr; Philip, Judge; Krucker, Sam
2016SPD....47.0613K    Altcode:
  The X1 flare on 2014-03-29 was observed with an unprecedented number
  of instruments including chromospheric polarimetry and spectroscopy
  from the UV to the IR. By combining data from these instruments, we can
  answer several open questions: Where is the observed continuum emission
  during flares formed and through which physical processes? How does
  the magnetic field structure in the photosphere and in the chromosphere
  change during a flare? We discuss the implications of our findings on
  standard flare models.

---------------------------------------------------------
Title: Is it Possible to Use the Green Coronal Line Instead of X rays
    to Cancel an Effect of the Coronal Emissivity Deficit in Estimation of
    the Prominence Total Mass from Decrease of the EUV-corona Intensities?
Authors: Schwartz, P.; Heinzel, P.; Jejčič, S.; Rybák, J.; Kotrč,
   P.; Fárník, F.; Kupryakov, Yu. A.; Deluca, E. E.; Golub, L.; Jibben,
   P. R.; Anzer, U.; Tlatov, A. G. .; Guseva, S. A.
2016ASPC..504...89S    Altcode:
  Total masses of six quiescent prominences observed from April through
  June 2011 were estimated using multi-spectral observations (in EUV,
  X-rays, Hα, and Ca &lt;small&gt;II&lt;/small&gt; H). The method for
  the total mass estimation is based on the fact that the intensity
  of the EUV solar corona at wavelengths below 912 Å is reduced at a
  prominence by the absorption in resonance continua (photoionisation)
  of hydrogen and possibly by helium and subsequently an amount of
  absorbed radiation is proportional to the column density of hydrogen
  and helium plasma. Moreover, the deficit of the coronal emissivity in
  volume occupied by the cool prominence plasma also contributes to the
  intensity decrease. The observations in X-rays which are not absorbed
  by the prominence plasma, allow us to separate these two mechanisms
  from each other. The X-ray observations of XRT onboard the Hinode
  satellite made with the Al-mesh focal filter were used because the
  X-ray coronal radiation formed in plasma of temperatures of the order
  of 10<SUP>6</SUP> K was registered and EUV spectral lines occurring in
  the 193, 211 and 335 Å channels of the Atmospheric Imaging Assembly
  of the Solar Dynamics Observatory satellite are also formed at such
  temperatures. Unfortunately, the Al-mesh filter has a secondary peak
  of the transmittance at around 171 Å which causes a contribution
  from the EUV corona to the measured data of up to 11 % in the quiet
  corona. Thus, absorption in prominence plasma influences XRT X-ray
  data when using the Al-mesh filter. On the other hand, other X-ray XRT
  filters are more sensitive to plasma of much higher temperatures (log
  T of the order of 7), thus observations using these filters cannot
  be used together with the AIA observations in the method for mass
  estimations. This problem could be solved using observations in the
  green coronal line instead of X-rays. Absorption of the green coronal
  line by a prominence plasma is negligible and this line is formed at
  temperatures of the order of 10<SUP>6</SUP> K. We compare values of
  the total mass of the prominence observed on 20 October 2012 on the
  SE limb estimated when using XRT X-ray observations and observations
  in the green coronal line obtained at Kislovodsk Mountain Astronomical
  Station of the Pulkovo observatory (Russia).

---------------------------------------------------------
Title: Magnetic Field and Plasma Diagnostics from Coordinated
    Prominence Observations
Authors: Schmieder, B.; Levens, P.; Dalmasse, K.; Mein, N.; Mein,
   P.; Lopez-Ariste, A.; Labrosse, N.; Heinzel, P.
2016ASPC..504..119S    Altcode:
  We study the magnetic field in prominences from a statistical point of
  view, by using THEMIS in the MTR mode, performing spectropolarimetry
  of the He I D<SUB>3</SUB> line. Combining these measurements with
  spectroscopic data from IRIS, Hinode/EIS as well as ground-based
  telescopes, such as the Meudon Solar Tower, we infer the temperature,
  density, and flow velocities of the plasma. There are a number of
  open questions that we aim to answer: - What is the general direction
  of the magnetic field in prominences? Is the model using a single
  orientation of magnetic field always valid for atypical prominences? %-
  Does this depend on the location of the filament on the disk (visible
  in Hα, in He II 304 Å) over an inversion line between weak or strong
  network ? - Are prominences in a weak environment field dominated by
  gas pressure? - Measuring the Doppler shifts in Mg II lines (with IRIS)
  and in Hα can tell us if there are substantial velocities to maintain
  vertical rotating structures, as has been suggested for tornado-like
  prominences. We present here some results obtained with different
  ground-based and space-based instruments in this framework.

---------------------------------------------------------
Title: Measurements of Continuum Flux in Solar Flares
Authors: Kotrč, P.; Heinzel, P.; Procházka, O.
2016ASPC..504...49K    Altcode:
  A broad-band diagnostics of chromospheric flare plasma needs to analyze
  spectra covering many spectral lines and various continuum features. The
  flare spectra are well detected on the background of the solar disk, but
  the detection of flare line emission from the Sun-as-a-star in optical
  is much more difficult due to a strong background radiation. When the
  flare/background radiation contrast is strong enough to be detected,
  we need a device for measuring the flux from a selected part of the
  flaring region. Here we present technical demands for such an instrument
  and its brief description. This device denoted as Image Selector is a
  post-focus instrument installed at the horizontal solar telescope HSFA2
  of the Ondřejov observatory, described by Kotrč (2009). Its core
  consists of a system of diaphragms, imaging Hα telescope and a fast
  spectrometer with dispersion of 3 px per Å but with cadency reaching
  up to 50 frames per second. The first solar flares observed recently
  by this novel technique provide quite interesting results. Our analysis
  of the data proves that the described device is sufficiently sensitive
  to detect variations in the Balmer continuum during solar flares.

---------------------------------------------------------
Title: Solar Science with the Atacama Large Millimeter/Submillimeter
    Array—A New View of Our Sun
Authors: Wedemeyer, S.; Bastian, T.; Brajša, R.; Hudson, H.;
   Fleishman, G.; Loukitcheva, M.; Fleck, B.; Kontar, E. P.; De Pontieu,
   B.; Yagoubov, P.; Tiwari, S. K.; Soler, R.; Black, J. H.; Antolin,
   P.; Scullion, E.; Gunár, S.; Labrosse, N.; Ludwig, H. -G.; Benz,
   A. O.; White, S. M.; Hauschildt, P.; Doyle, J. G.; Nakariakov, V. M.;
   Ayres, T.; Heinzel, P.; Karlicky, M.; Van Doorsselaere, T.; Gary,
   D.; Alissandrakis, C. E.; Nindos, A.; Solanki, S. K.; Rouppe van
   der Voort, L.; Shimojo, M.; Kato, Y.; Zaqarashvili, T.; Perez, E.;
   Selhorst, C. L.; Barta, M.
2016SSRv..200....1W    Altcode: 2015SSRv..tmp..118W; 2015arXiv150406887W
  The Atacama Large Millimeter/submillimeter Array (ALMA) is a new
  powerful tool for observing the Sun at high spatial, temporal, and
  spectral resolution. These capabilities can address a broad range
  of fundamental scientific questions in solar physics. The radiation
  observed by ALMA originates mostly from the chromosphere—a complex
  and dynamic region between the photosphere and corona, which plays a
  crucial role in the transport of energy and matter and, ultimately,
  the heating of the outer layers of the solar atmosphere. Based on
  first solar test observations, strategies for regular solar campaigns
  are currently being developed. State-of-the-art numerical simulations
  of the solar atmosphere and modeling of instrumental effects can help
  constrain and optimize future observing modes for ALMA. Here we present
  a short technical description of ALMA and an overview of past efforts
  and future possibilities for solar observations at submillimeter and
  millimeter wavelengths. In addition, selected numerical simulations
  and observations at other wavelengths demonstrate ALMA's scientific
  potential for studying the Sun for a large range of science cases.

---------------------------------------------------------
Title: Non-LTE Inversion of Spectropolarimetric and Spectroscopic
    Observations of a Small Active-region Filament Observed at the VTT
Authors: Schwartz, P.; Balthasar, H.; Kuckein, C.; Koza, J.; Gömöry,
   P.; Rybák, J.; Kučera, A.; Heinzel, P.
2016ASPC..504..205S    Altcode:
  An active region mini-filament was observed by VTT simultaneously
  in the He&lt;small&gt;I&lt;/small&gt; 10 830 Å triplet by the TIP 1
  spectropolarimeter, in Hα by the TESOS Fabry-Pérot interferometer, and
  in Ca &lt;small&gt;II&lt;/small&gt; 8542 Å by the VTT spectrograph. The
  spectropolarimetric data were inverted using the HAZEL code and Hα
  profiles were modelled solving a NLTE radiative transfer in a simple
  isobaric and isothermal 2D slab irradiated both from bottom and
  sides. It was found that the mini-filament is composed of horizontal
  fluxtubes, along which the cool plasma of T∼10 000 K can flow by
  very large - even supersonic - velocities.

---------------------------------------------------------
Title: New Observations of Balmer Continuum Flux in Solar
    Flares. Instrument Description and First Results
Authors: Kotrč, P.; Procházka, O.; Heinzel, P.
2016SoPh..291..779K    Altcode: 2016SoPh..tmp...17K; 2016arXiv160104610K
  Increase in the Balmer continuum radiation during solar flares was
  predicted by various authors, but has never been firmly confirmed
  observationally using ground-based slit spectrographs. Here we
  describe a new post-focal instrument, the image selector, with which
  the Balmer continuum flux can be measured from the whole flare area,
  in analogy to successful detections of flaring dMe stars. The system
  was developed and put into operation at the horizontal solar telescope
  HSFA2 of the Ondřejov Observatory. We measure the total flux by a
  fast spectrometer from a limited but well-defined region on the solar
  disk. Using a system of diaphragms, the disturbing contribution of a
  bright solar disk can be eliminated as much as possible. Light curves
  of the measured flux in the spectral range 350 - 440 nm are processed,
  together with the H α images of the flaring area delimited by the
  appropriate diaphragm. The spectral flux data are flat-fielded,
  calibrated, and processed to be compared with model predictions. Our
  analysis of the data proves that the described device is sufficiently
  sensitive to detect variations in the Balmer continuum during solar
  flares. Assuming that the Balmer-continuum kernels have at least a
  similar size as those visible in H α , we find the flux increase in
  the Balmer continuum to reach 230 - 550 % of the quiet continuum during
  the observed X-class flare. We also found temporal changes in the Balmer
  continuum flux starting well before the onset of the flare in H α.

---------------------------------------------------------
Title: Observations and modeling of the ultraviolet emission of
    solar flares
Authors: Mikuła, Katarzyna; Berlicki, Arkadiusz; Heinzel, Petr
2016IAUS..320...57M    Altcode:
  In this paper we present the method of using far UV spectra of
  the flare observed by Interface Region Imaging Spectrograph (IRIS)
  for determination of the contribution of the continuum emission to
  the total UV radiation observed e.g. by SDO in 1600 Å channel. In
  our method the Si IV (1402.77 Å) line observed by IRIS is used as a
  proxy of C IV line emission contained in SDO/AIA UV images. Determined
  intensity of the flare continuum emission can be used to study the
  physics of the flare heated chromosphere and for better understanding
  of the emission mechanisms.

---------------------------------------------------------
Title: White-light continuum emission from a solar flare and plage
Authors: Berlicki, Arkadiusz; Awasthi, Arun Kumar; Heinzel, Petr;
   Sobotka, Michal
2016IAUS..320..268B    Altcode: 2016arXiv160404186B
  Observations of flare emissions in the optical continuum are very
  rare. Therefore, the analysis of such observations is useful and
  may contribute to our understanding of the flaring chromosphere and
  photosphere. We study the white light continuum emission observed
  during the X6.9 flare. This emission comes not only from the flare
  ribbons but also form the nearby plage area. The main aim of this work
  is to disentangle the flare and plage (facula) emission. We analyzed
  the spatial, spectral and temporal evolution of the flare and plage
  properties by analyzing multi-wavelength observations. We study
  the morphological correlation of the white-light continuum emission
  observed with different instruments. We found that some active region
  areas which produce the continuum emission correspond rather to plages
  than to the flare kernels. We showed that in some cases the continuum
  emission from the WL flare kernels is very similar to the continuum
  emission of faculae.

---------------------------------------------------------
Title: Numerical RHD simulations of flaring chromosphere with Flarix
Authors: Heinzel, Petr; Kašparová, Jana; Varady, Michal; Karlický,
   Marian; Moravec, Zdeněk
2016IAUS..320..233H    Altcode: 2016arXiv160200016H
  Flarix is a radiation-hydrodynamical (RHD) code for modeling of the
  response of the chromosphere to a beam bombardment during solar
  flares. It solves the set of hydrodynamic conservation equations
  coupled with NLTE equations of radiative transfer. The simulations are
  driven by high energy electron beams. We present results of the Flarix
  simulations of a flaring loop relevant to the problem of continuum
  radiation during flares. In particular we focus on properties of the
  hydrogen Balmer continuum which was recently detected by IRIS.

---------------------------------------------------------
Title: Continuum Enhancements in the Ultraviolet, the Visible and
    the Infrared during the X1 Flare on 2014 March 29
Authors: Kleint, Lucia; Heinzel, Petr; Judge, Phil; Krucker, Säm
2016ApJ...816...88K    Altcode: 2015arXiv151104161K
  Enhanced continuum brightness is observed in many flares (“white
  light flares”), yet it is still unclear which processes contribute to
  the emission. To understand the transport of energy needed to account
  for this emission, we must first identify both the emission processes
  and the emission source regions. Possibilities include heating in the
  chromosphere causing optically thin or thick emission from free-bound
  transitions of Hydrogen, and heating of the photosphere causing enhanced
  H<SUP>-</SUP> continuum brightness. To investigate these possibilities,
  we combine observations from Interface Region Imaging Spectrograph
  (IRIS), SDO/Helioseismic and Magnetic Imager, and the ground-based
  Facility Infrared Spectrometer instrument, covering wavelengths in
  the far-UV, near-UV (NUV), visible, and infrared during the X1 flare
  SOL20140329T17:48. Fits of blackbody spectra to infrared and visible
  wavelengths are reasonable, yielding radiation temperatures ∼6000-6300
  K. The NUV emission, formed in the upper photosphere under undisturbed
  conditions, exceeds these simple fits during the flare, requiring
  extra emission from the Balmer continuum in the chromosphere. Thus,
  the continuum originates from enhanced radiation from photosphere
  (visible-IR) and chromosphere (NUV). From the standard thick-target
  flare model, we calculate the energy of the nonthermal electrons
  observed by Reuven Ramaty High Energy Solar Spectroscope Imager (RHESSI)
  and compare it to the energy radiated by the continuum emission. We
  find that the energy contained in most electrons &gt;40 keV, or
  alternatively, of ∼10%-20% of electrons &gt;20 keV is sufficient to
  explain the extra continuum emission of ∼(4-8) × 10<SUP>10</SUP>
  erg s<SUP>-1</SUP> cm<SUP>-2</SUP>. Also, from the timing of the RHESSI
  HXR and the IRIS observations, we conclude that the NUV continuum is
  emitted nearly instantaneously when HXR emission is observed with a
  time difference of no more than 15 s.

---------------------------------------------------------
Title: Lines of MgI Detected in Solar Prominences
Authors: Heinzel, P.; Kupryakov, Yu.; Schwartz, P.
2016CEAB...40...87H    Altcode:
  Using the flare spectrograph at Ondřejov observatory, we have observed
  several prominences with the aim to detect the MgI lines. These lines
  play an important diagnostic role, complementary to MgII resonance
  lines now routinely observed by the IRIS satellite. Our preliminary
  analysis shows that a rather weak MgI emission, e.g. in the 5172.7
  Å line, is detectable and this correlates well with the presence of
  extended bright regions on the solar disk visible in SDO/AIA 1600 Å
  band. Physical reasons for such a correlation are discussed.

---------------------------------------------------------
Title: Observed IRIS Profiles of the h and k Doublet of Mg II and
    Comparison with Profiles from Quiescent Prominence NLTE Models
Authors: Vial, Jean-Claude; Pelouze, Gabriel; Heinzel, Petr; Kleint,
   Lucia; Anzer, Ulrich
2016SoPh..291...67V    Altcode: 2015SoPh..tmp..173V
  With the launch of the Interface Region Imaging Spectrograph (IRIS)
  mission, it is now possible to obtain high-resolution solar prominence
  spectra and to begin to distinguish the contributions of the many
  (apparent or not) threads that structure prominences. We aim at
  comparing unique observations obtained in the Mg II h and k lines of a
  polar crown prominence with the radiative outputs from one-dimensional
  models built with non-local-thermodynamic equilibrium codes (Heinzel et
  al.Astron. Astrophys.564, A132, 2014). We characterize the profiles
  obtained through thorough calibration procedures, with attention
  paid to the absolute values, full-width at half-maximum, and the
  ratio of k to h intensities. We also show that at the top of some
  structures, line-of-sight velocities of about 9 kms−<SUP>1</SUP> can
  be detected. We find a range of static, low-pressure, low-thickness,
  low-temperature models that could fit k or h observed values, but that
  cannot satisfy the low observed k/h ratio. We investigate whether these
  low values might be explained by the inclusion of horizontal flows in
  small-scale threads. These flows are also necessary in another class
  of models, where the pressure is kept low but thickness and temperature
  are increased up to the observed thickness and up to 15 000 K.

---------------------------------------------------------
Title: Solar and Stellar Flares and their Effects on Planets
Authors: Kosovichev, A. G.; Hawley, S. L.; Heinzel, P.
2016IAUS..320.....K    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: SSALMON - The Solar Simulations for the Atacama Large
    Millimeter Observatory Network
Authors: Wedemeyer, S.; Bastian, T.; Brajša, R.; Barta, M.; Hudson,
   H.; Fleishman, G.; Loukitcheva, M.; Fleck, B.; Kontar, E.; De Pontieu,
   B.; Tiwari, S.; Kato, Y.; Soler, R.; Yagoubov, P.; Black, J. H.;
   Antolin, P.; Gunár, S.; Labrosse, N.; Benz, A. O.; Nindos, A.;
   Steffen, M.; Scullion, E.; Doyle, J. G.; Zaqarashvili, T.; Hanslmeier,
   A.; Nakariakov, V. M.; Heinzel, P.; Ayres, T.; Karlicky, M.
2015AdSpR..56.2679W    Altcode: 2015arXiv150205601W
  The Solar Simulations for the Atacama Large Millimeter Observatory
  Network (SSALMON) was initiated in 2014 in connection with two ALMA
  development studies. The Atacama Large Millimeter/submillimeter Array
  (ALMA) is a powerful new tool, which can also observe the Sun at
  high spatial, temporal, and spectral resolution. The international
  SSALMONetwork aims at co-ordinating the further development of solar
  observing modes for ALMA and at promoting scientific opportunities
  for solar physics with particular focus on numerical simulations,
  which can provide important constraints for the observing modes and
  can aid the interpretation of future observations. The radiation
  detected by ALMA originates mostly in the solar chromosphere - a
  complex and dynamic layer between the photosphere and corona, which
  plays an important role in the transport of energy and matter and the
  heating of the outer layers of the solar atmosphere. Potential targets
  include active regions, prominences, quiet Sun regions, flares. Here,
  we give a brief overview over the network and potential science cases
  for future solar observations with ALMA.

---------------------------------------------------------
Title: Preface
Authors: Fletcher, L.; Heinzel, P.; van Driel-Gesztelyi, L.; Mandrini,
   C. H.; Fárník, F.
2015SoPh..290.3379F    Altcode: 2015SoPh..tmp..168F
  No abstract at ADS

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Title: Mg II Lines Observed During the X-class Flare on 29 March
    2014 by the Interface Region Imaging Spectrograph
Authors: Liu, W.; Heinzel, P.; Kleint, L.; Kašparová, J.
2015SoPh..290.3525L    Altcode: 2015SoPh..tmp..166L; 2015arXiv151100480L
  Mg II lines represent one of the strongest emissions from the
  chromospheric plasma during solar flares. In this article, we
  studied the Mg II lines observed during the X1 flare on 29 March 2014
  (SOL2014-03-29T17:48) by the Interface Region Imaging Spectrograph
  (IRIS). IRIS detected large intensity enhancements of the Mg II h and
  k lines, subordinate triplet lines, and several other metallic lines
  at the flare footpoints during this flare. We have used the advantage
  of the slit-scanning mode (rastering) of IRIS and performed, for the
  first time, a detailed analysis of spatial and temporal variations
  of the spectra. Moreover, we were also able to identify positions
  of strongest hard X-ray (HXR) emissions using the Reuven Ramaty
  High Energy Solar Spectroscopic Imager (RHESSI) observations and to
  correlate them with the spatial and temporal evolution of IRIS Mg
  II spectra. The light curves of the Mg II lines increase and peak
  contemporarily with the HXR emissions but decay more gradually. There
  are large red asymmetries in the Mg IIh and k lines after the flare
  peak. We see two spatially well-separated groups of Mg II line profiles,
  non-reversed and reversed. In some cases, the Mg II footpoints with
  reversed profiles are correlated with HXR sources. We show the spatial
  and temporal behavior of several other line parameters (line metrics)
  and briefly discuss them. Finally, we have synthesized the Mg IIk line
  using our non-LTE code with the Multilevel Accelerated Lambda Iteration
  (MALI) technique. Two kinds of models are considered, the flare model
  F2 of Machado et al. (Astrophys. J.242, 336, 1980) and the models of
  Ricchiazzi and Canfield (Astrophys. J.272, 739, 1983, RC models). Model
  F2 reproduces the peak intensity of the non-reversed Mg IIk profile
  at flare maximum, but does not account for high wing intensities. On
  the other hand, the RC models show the sensitivity of Mg II line
  intensities to various electron-beam parameters. Our simulations also
  show that the microturbulence produces a broader line core, while the
  intense line wings are caused by an enhanced line source function.

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Title: White-light continuum emission from solar flare and plages:
    observations and modeling
Authors: Berlicki, Arkadiusz; Awasthi, Arun Kumar; Heinzel, Petr
2015IAUGA..2256469B    Altcode:
  Observations of flares in optical continuum emission are very
  rare. Therefore, the analysis of such observations is very useful and
  may contribute to our understanding of the flaring chromosphere. We
  study the white-light continuum emission observed during the X6.9
  flare observed on August 09, 2011. This emission comes not only from
  the flare ribbons but also form the nearby plage area observed within
  the active region. The main aim of this work is to disentangle the
  flare and plage emission and to understand the physical mechanisms
  responsible for the production of white-light continuum.There are two
  main mechanisms which can be responsible for the optical continuum
  emission of the solar atmosphere: enhanced photospheric H- continuum
  due to the temperature increase below the temperature minimum region,
  or hydrogen recombination continua (Balmer, Paschen) formed in solar
  chromosphere. In our work we analyse the physical conditions in solar
  active atmosphere in order to obtain the contribution from these two
  mechanisms to the whole continuum emission of the flare and plage.We
  analyzed the spatial, spectral and temporal evolution study of the
  flare and plage parameters by analyzing multi-wavelength observations
  obtained from ground and space based solar observatories. We study
  the morphological correlation of the white-light continuum emission
  observed with different instruments. Moreover, we also explore the
  non-thermal electron beam properties by forward fitting the observed
  X-ray spectra.The unique opportunity of an intense X6.9 flare occurrence
  close to the limb enabled us to explore the origin of white-light
  continuum with better visibility. The analysis of multi-wavelength
  data revealed the origin of this emission from the foot-points of the
  loops. Spatial association of HXR foot-points synthesized from RHESSI
  observations confirmed this finding. In addition, we found a good
  temporal correlation of hard (&gt;30 keV) X-ray with the white-light
  emission. However, some active region areas which produce the continuum
  emission correspond rather to plages than to the flare kernels.

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Title: Multi-wavelength diagnostics and modelling of the emission
    during a B6.4 flare of August 20, 2005
Authors: Awasthi, Arun Kumar; Berlicki, Arkadiusz; Rudawy, Powel;
   Heinzel, Petr
2015IAUGA..2256580A    Altcode:
  We study the temporal, spatial and spectral evolution of
  multi-wavelength emission observed during a B6.4 flare occurred
  on August 20, 2005 with the motivation to outline the thermal and
  non-thermal processes during the precursor and gradual phase of the
  flare. Precursor phase is designated as the gradual enhancement of
  soft X-ray emission prior to onset of the impulsive phase. Observations
  from several space and ground based observatories viz. RHESSI, TRACE,
  GONG, SoHO/EIT and NoRP are included in this study. Temporal evolution
  of X-ray emission does not show the presence of hard X-rays (&gt;12
  keV) emission during the precursor phase of the flare. We synthesized
  X-ray images in 6-12 keV from RHESSI observations, which show several
  discrete sources during the precursor phase. Following to this, one
  of these sources pronounced during the main phase of the flare. We
  carry out in-depth analysis of chromospheric response in various
  phases of the flare employing high temporal cadence images of the Sun
  in Hα line centre as well as wings obtained from the Multi-channel
  Subtractive Double Pass Spectrograph (MSDP) at the Bialkow Observatory
  of the University of Wroclaw, Poland. Our analysis of Hα images
  during the main phase of the flare suggests localized emission in
  the form of kernels. On the contrary, we note extended and diffused
  source morphology of emitting region during the precursor phase of
  the flare. We also study various kinematic properties of different
  structures visible in the Hα images in the line centre as well as
  wings. In addition, the correlation of the relative timing of X-ray
  and Hα emission profile is performed to estimate the delay in the
  chromospheric response during different phases of flare. Further, we
  employ thermal plasma parameters estimated during the precursor and
  gradual phase to model the associated Hα emission. For the modeling we
  employ NLTE numerical codes modified for flare conditions. The modeled
  and observed flare emission parameters are then compared. Finally,
  we propose a unified schematic scenario for the trigger and energy
  release during this low-intensity class flare.

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Title: Observations and modeling of the ultraviolet emission of
    solar flares
Authors: Berlicki, Arkadiusz; Heinzel, Petr; Mikula, Katarzyna
2015IAUGA..2257337B    Altcode:
  It is well known that during solar flares the heated chromospheric
  plasma emits the ultraviolet (UV) radiation in spectral lines
  and continua. UV space telescopes (e.g. TRACE, Solar Dynamic
  Observatory/Atmospheric Imaging Assembly - SDO/AIA) provide images
  of solar flares where the complicated fine structure of the flaring
  atmosphere is well visible. However, these broadband images contain
  the mixture of line and continuum UV emission and it is not possible
  to disentangle between these two contributions. E.g. solar flare
  brightening observed in SDO/AIA 160 nm channel can be visible both due
  to the strong line emission in C IV 154.8 nm or due to the continuum
  increase. Spectral lines and continua are formed in plasma of different
  temperature and location. Therefore, in order to obtain the parameters
  of plasma we should know quantitatively the contribution from lines and
  continua.Such analysis would be possible using the UV spectrograph,
  where we can see the intensity of lines and continua separately. For
  example Interface Region Imaging Spectrograph (IRIS) provides such
  spectra of flares, where the enhanced lines and continuum is visible
  both in NUV (near UV) and FUV (far UV) channels.In our work we used
  IRIS flare observations in FUV channel to determine the intensity of
  spectral lines, including Si IV 139.4 nm line. Then, using CHIANTI
  procedures and the observed intensities of some FUV lines we computed
  the synthetic UV spectrum for given flare model. IRIS spectrum does not
  include C IV line, which contaminates the SDO/AIA images, but this line
  can be calculated in the theoretical CHIANTI spectrum. In this way, we
  can subtract the C IV (and other lines) emission from SDO/AIA images and
  obtain the pure UV continuum intensity. Finally, the obtained continuum
  emission can used to study the physics of heated chromosphere of flares.

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Title: High-resolution fine-structure synthetic imaging of an entire
    prominence using 3D whole-prominence fine structure modelling
Authors: Gunar, Stanislav; Mackay, Duncan; Heinzel, Petr; Anzer, Ulrich
2015IAUGA..2251323G    Altcode:
  The newly developed 3D whole-prominence fine structure (WPFS)
  model (Gunár &amp; Mackay 2015) allows us for the first time to
  simulate entire prominences/filaments including their numerous fine
  structures. This model combines a 3D magnetic field configuration of an
  entire prominence obtained from non-linear force-free field simulations,
  with a detailed description of the prominence plasma. The plasma is
  located in magnetic dips in hydrostatic equilibrium and is distributed
  along hundreds of fine structures within the 3D magnetic model. The
  prominence plasma has realistic density and temperature distributions
  including the prominence-corona transition region.To produce the
  high-resolution synthetic H-alpha images of the WPFS model we use
  a novel fast approximate radiative transfer visualization technique
  (Heinzel et al. 2015). This allows us for the first time to produce
  images of the prominences in emission on the solar limb and filaments in
  absorption against the solar disk using a single model. The prominence
  plasma and magnetic field are described in the WPFS model on scales
  that allow us to produce synthetic images with resolution matching that
  of the state-of-the-art observations, or indeed that of the upcoming
  solar observatories, such as DKIST or Solar-C. Moreover, to complement
  the prominence/filament synthetic images we have consistent information
  about the magnetic field and plasma parameters everywhere in the modeled
  prominences. This allows us to investigate the apparent puzzling nature
  of the observed prominence and filament fine structures. We can also
  study the connections between the local configuration of the magnetic
  field and the observable structure of the finest prominence/filament
  features. In addition, we are able to investigate the prominence
  evolution. We can consistently study the influence of the varying
  photospheric flux distribution on the prominence magnetic field
  configuration and its effect on the observable prominence plasma.

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Title: On the Visibility of Prominence Fine Structures at Radio
    Millimeter Wavelengths
Authors: Heinzel, P.; Berlicki, A.; Bárta, M.; Karlický, M.;
   Rudawy, P.
2015SoPh..290.1981H    Altcode: 2015SoPh..tmp...87H
  Prominence temperatures have so far mainly been determined by analyzing
  spectral line shapes, which is difficult when the spectral lines are
  optically thick. The radio spectra in the millimeter range offer
  a unique possibility to measure the kinetic temperature. However,
  studies in the past used data with insufficient spatial resolution
  to resolve the prominence fine structures. The aim of this article
  is to predict the visibility of prominence fine structures in the
  submillimeter/millimeter (SMM) domain, to estimate their brightness
  temperatures at various wavelengths, and to demonstrate the feasibility
  and usefulness of future high-resolution radio observations of
  solar prominences with ALMA (Atacama Large Millimeter-submillimeter
  Array). Our novel approach is the conversion of Hα coronagraphic images
  into microwave spectral images. We show that the spatial variations
  of the prominence brightness both in the Hα line and in the SMM
  domain predominantly depend on the line-of-sight emission measure of
  the cool plasma, which we derive from the integrated intensities of
  the observed Hα line. This relation also offers a new possibility to
  determine the SMM optical thickness from simultaneous Hα observations
  with high resolution. We also describe how we determine the prominence
  kinetic temperature from SMM spectral images. Finally, we apply the
  ALMA image-processing software Common Astronomy Software Applications
  (CASA) to our simulated images to assess what ALMA would detect at a
  resolution level that is similar to the coronagraphic Hα images used
  in this study. Our results can thus help in preparations of first
  ALMA prominence observations in the frame of science and technical
  verification tests.

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Title: Fast approximate radiative transfer method for visualizing
    the fine structure of prominences in the hydrogen Hα line
Authors: Heinzel, P.; Gunár, S.; Anzer, U.
2015A&A...579A..16H    Altcode:
  <BR /> Aims: We present a novel approximate radiative transfer method
  developed to visualize 3D whole-prominence models with multiple fine
  structures using the hydrogen Hα spectral line. <BR /> Methods: This
  method employs a fast line-of-sight synthesis of the Hα line profiles
  through the whole 3D prominence volume and realistically reflects the
  basic properties of the Hα line formation in the cool and low-density
  prominence medium. The method can be applied both to prominences seen
  above the limb and filaments seen against the disk. <BR /> Results:
  We provide recipes for the use of this method for visualizing the
  prominence or filament models that have multiple fine structures. We
  also perform tests of the method that demonstrate its accuracy
  under prominence conditions. <BR /> Conclusions: We demonstrate that
  this fast approximate radiative transfer method provides realistic
  synthetic Hα intensities useful for a reliable visualization of
  prominences and filaments. Such synthetic high-resolution images of
  modeled prominences/filaments can be used for a direct comparison with
  high-resolution observations.

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Title: Prominence Visibility in Hinode/XRT Images
Authors: Schwartz, P.; Jejčič, S.; Heinzel, P.; Anzer, U.; Jibben,
   P. R.
2015ApJ...807...97S    Altcode: 2015arXiv150606078S
  In this paper we study the soft X-ray (SXR) signatures of one
  particular prominence. The X-ray observations used here were made by the
  Hinode/X-Ray Telescope instrument using two different filters. Both of
  them have a pronounced peak of the response function around 10 Å. One
  of them has a secondary smaller peak around 170 Å, which leads to a
  contamination of SXR images. The observed darkening in both of these
  filters has a very large vertical extension. The position and shape of
  the darkening correspond nicely with the prominence structure seen in
  SDO/AIA images. First, we have investigated the possibility that the
  darkening is caused by X-ray absorption. However, detailed calculations
  of the optical thickness in this spectral range show clearly that
  this effect is completely negligible. Therefore, the alternative is
  the presence of an extended region with a large emissivity deficit,
  which can be caused by the presence of cool prominence plasmas within
  an otherwise hot corona. To reproduce the observed darkening, one needs
  a very large extension along the line of sight of the region amounting
  to around 10<SUP>5</SUP> km. We interpret this region as the prominence
  spine, which is also consistent with SDO/AIA observations in EUV.

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Title: Understanding the Mg II and Hα Spectra in a Highly Dynamical
    Solar Prominence
Authors: Heinzel, P.; Schmieder, B.; Mein, N.; Gunár, S.
2015ApJ...800L..13H    Altcode:
  Mg ii h and k and Hα spectra in a dynamical prominence have been
  obtained along the slit of the Interface Region Imaging Spectrograph
  (IRIS) and with the Meudon Multi-channel Subtractive Double Pass
  spectrograph on 2013 September 24, respectively. Single Mg ii line
  profiles are not much reversed, while at some positions along
  the IRIS slit the profiles show several discrete peaks that are
  Doppler-shifted. The intensity of these peaks is generally decreasing
  with their increasing Doppler shift. We interpret this unusual behavior
  as being due to the Doppler dimming effect. We discuss the possibility
  to interpret the unreversed single profiles by using a two-dimensional
  (2D) model of the entire prominence body with specific radiative
  boundary conditions. We have performed new 2D isothermal-isobaric
  modeling of both Hα and Mg ii lines and show the ability of such models
  to account for the line profile variations as observed. However, the Mg
  ii line-center intensities require the model with a temperature increase
  toward the prominence boundary. We show that even simple one-dimensional
  (1D) models with a prominence-to-corona transition region (PCTR) fit the
  observed Mg ii and Hα lines quite well, while the isothermal-isobaric
  models (1D or 2D) are inconsistent with simultaneous observations in
  the Mg ii h and k and Hα lines, meaning that the Hα line provides a
  strong additional constraint on the modeling. IRIS far-UV detection of
  the C ii lines in this prominence seems to provide a direct constraint
  on the PCTR part of the model.

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Title: Total mass of six quiescent prominences estimated from their
    multi-spectral observations
Authors: Schwartz, P.; Heinzel, P.; Kotrč, P.; Fárník, F.;
   Kupryakov, Yu. A.; DeLuca, E. E.; Golub, L.
2015A&A...574A..62S    Altcode:
  Context. Total masses of six solar prominences were estimated using
  prominence multi-spectral observations (in EUV, X-rays, Hα, and Ca
  ii H). The observations were made during the observing campaign from
  April through June 2011. <BR /> Aims: The aim of the work was to apply
  a complex method for the prominence mass estimations that can be used
  later for other prominences observed during the observing campaign. <BR
  /> Methods: Our method is based on the fact that intensity of the EUV
  solar corona at wavelengths below 912 Å is reduced by the absorption
  in resonance continua of hydrogen and helium (photoionisation) and at
  the same time also by a deficit of the coronal emissivity in volume
  occupied by the cool prominence plasma. Both mechanisms contribute to
  intensity decrease simultaneously. The observations in X-rays allow us
  to separate these mechanisms from each other. Coronal emission behind a
  prominence is not estimated by any temporal or spatial interpolation,
  but by using a new method based on comparing the ratio of the optical
  thickness at 193 Å and 211 Å determined from the observations
  with the theoretical ratio. <BR /> Results: Values of the total mass
  estimated for six prominences are between 2.9 × 10<SUP>11</SUP> and
  1.7 × 10<SUP>12</SUP> kg. The column density of hydrogen is of the
  order of 10<SUP>18</SUP>-10<SUP>19</SUP> cm<SUP>-2</SUP>. Our results
  agree with results of other authors. <BR /> Conclusions: The method
  is now ready to be used for all 30 prominences observed during the
  campaign. Then in the near future it will be possible to obtain a
  statistics of the total mass of quiescent solar prominences.

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Title: Radiative Transfer in Solar Prominences
Authors: Heinzel, Petr
2015ASSL..415..103H    Altcode:
  Critical information about prominence physical conditions can be
  obtained only by analyzing prominence spectra or high-resolution
  monochromatic images. Solar prominences are low-density structures
  and, therefore, the non-equilibrium (NLTE) spectroscopy tools have
  to be used. We describe the basics of the NLTE radiative-transfer
  theory applied to typical prominence conditions and demonstrate why
  the NLTE approach is necessary. Starting from the simplest 1D slab
  models, we gradually move to more complex problems which include 2D
  transfer, importance of partial redistribution in the formation of
  resonance lines and details of multilevel problems including the most
  up-to-date numerical methods for constructing NLTE models. We also
  mention some recent achievements in prominence modeling (e.g. magnetic
  dips, radiative equilibrium models, oscillations), although detailed
  description of such results is the subject of other chapters.

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Title: On the Origin of Linear Polarization in Solar Flares
Authors: Štěpán, J.; Heinzel, P.
2014ASPC..489..133S    Altcode:
  A significant degree of linear polarization (up to few percent) of
  some spectral lines is occasionally reported from the observations of
  solar flares. This polarization is often found at the edges of the
  flare ribbons and it is usually radial or tangential. The mechanism
  usually considered as being responsible for this effect is the
  impact polarization by electron and/or proton beams bombarding the
  chromosphere. We point out that resonant scattering polarization in a
  multi-dimensional geometry of the chromosphere has to be considered as
  an important ingredient of the problem. The significant horizontal
  inhomogeneities at the boundaries of the flare ribbons causes a
  considerable change in the radiation field anisotropy which may lead
  to emission of strongly linearly polarized spectral lines. For more
  details see Štěpán, &amp; Heinzel (2013)

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Title: Hydrogen Balmer Continuum in Solar Flares Detected by the
    Interface Region Imaging Spectrograph (IRIS)
Authors: Heinzel, P.; Kleint, L.
2014ApJ...794L..23H    Altcode: 2014arXiv1409.5680H
  We present a novel observation of the white light flare (WLF) continuum,
  which was significantly enhanced during the X1 flare on 2014 March
  29 (SOL2014-03-29T17:48). Data from the Interface Region Imaging
  Spectrograph (IRIS) in its near-UV channel show that at the peak of
  the continuum enhancement, the contrast at the quasi-continuum window
  above 2813 Å reached 100%-200% and can be even larger closer to Mg
  II lines. This is fully consistent with the hydrogen recombination
  Balmer-continuum emission, which follows an impulsive thermal and
  non-thermal ionization caused by the precipitation of electron beams
  through the chromosphere. However, a less probable photospheric
  continuum enhancement cannot be excluded. The light curves of the
  Balmer continuum have an impulsive character with a gradual fading,
  similar to those detected recently in the optical region on the
  Solar Optical Telescope on board Hinode. This observation represents
  a first Balmer-continuum detection from space far beyond the Balmer
  limit (3646 Å), eliminating seeing effects known to complicate the
  WLF detection. Moreover, we use a spectral window so far unexplored
  for flare studies, which provides the potential to study the Balmer
  continuum, as well as many metallic lines appearing in emission
  during flares. Combined with future ground-based observations of the
  continuum near the Balmer limit, we will be able to disentangle various
  scenarios of the WLF origin. IRIS observations also provide a critical
  quantitative measure of the energy radiated in the Balmer continuum,
  which constrains various models of the energy transport and deposit
  during flares.

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Title: Multi-Wavelength Eclipse Observations of a Quiescent Prominence
Authors: Jejčič, S.; Heinzel, P.; Zapiór, M.; Druckmüller, M.;
   Gunár, S.; Kotrč, P.
2014SoPh..289.2487J    Altcode: 2014SoPh..tmp...30J
  We construct the maps of temperatures, geometrical thicknesses,
  electron densities and gas pressures in a quiescent prominence. For
  this we use the RGB signal of the prominence visible-light emission
  detected during the total solar eclipse of 1 August 2008 in Mongolia
  and quasi-simultaneous Hα spectra taken at Ondřejov Observatory. The
  method of disentangling the electron density and geometrical (effective)
  thickness was described by Jejčič and Heinzel (Solar Phys.254,
  89 - 100, 2009) and is used here for the first time to analyse
  the spatial variations of prominence parameters. For the studied
  prominence we obtained the following range of parameters: temperature
  6000 - 15 000 K, effective thickness 200 - 15000 km, electron density
  5×10<SUP>9</SUP> - 10<SUP>11</SUP> cm<SUP>−3</SUP> and gas pressure
  0.02 - 0.2 dyn cm<SUP>−2</SUP> (assuming a fixed ionisation degree
  n<SUB>p</SUB>/n<SUB>H</SUB>=0.5). The electron density increases
  towards the bottom of the prominence, which we explain by an enhanced
  photoionisation due to the incident solar radiation. To confirm this,
  we construct a two-dimensional radiative-transfer model with realistic
  prominence illumination.

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Title: Observations and NLTE modeling of Ellerman bombs
Authors: Berlicki, A.; Heinzel, P.
2014A&A...567A.110B    Altcode: 2014arXiv1406.5702B
  Context. Ellerman bombs (EBs) are short-lived, compact, and spatially
  well localized emission structures that are observed well in the wings
  of the hydrogen Hα line. EBs are also observed in the chromospheric
  CaII lines and in UV continua as bright points located within active
  regions. Hα line profiles of EBs show a deep absorption at the line
  center and enhanced emission in the line wings with maxima around
  ±1 Å from the line center. Similar shapes of the line profiles are
  observed for the CaII IR line at 8542 Å. In CaII H and K lines the
  emission peaks are much stronger, and EBs emission is also enhanced
  in the line center. <BR /> Aims: It is generally accepted that
  EBs may be considered as compact microflares located in lower solar
  atmosphere that contribute to the heating of these low-lying regions,
  close to the temperature minimum of the atmosphere. However, it is
  still not clear where exactly the emission of EBs is formed in the
  solar atmosphere. High-resolution spectrophotometric observations
  of EBs were used for determining of their physical parameters and
  construction of semi-empirical models. Obtained models allow us to
  determine the position of EBs in the solar atmosphere, as well as
  the vertical structure of the activated EB atmosphere <BR /> Methods:
  In our analysis we used observations of EBs obtained in the Hα and
  CaII H lines with the Dutch Open Telescope (DOT). These one-hour
  long simultaneous sequences obtained with high temporal and spatial
  resolution were used to determine the line emissions. To analyze them,
  we used NLTE numerical codes for the construction of grids of 243
  semi-empirical models simulating EBs structures. In this way, the
  observed emission could be compared with the synthetic line spectra
  calculated for all such models. <BR /> Results: For a specific model
  we found reasonable agreement between the observed and theoretical
  emission and thus we consider such model as a good approximation to EBs
  atmospheres. This model is characterized by an enhanced temperature in
  the lower chromosphere and can be considered as a compact structure (hot
  spot), which is responsible for the emission observed in the wings of
  chromospheric lines, in particular in the Hα and CaII H lines. <BR />
  Conclusions: For the first time the set of two lines Hα and CaII H was
  used to construct semi-empirical models of EBs. Our analysis shows that
  EBs can be described by a "hot spot" model, with the temperature and/or
  density increase through a few hundred km atmospheric structure. We
  confirmed that EBs are located close to the temperature minimum or
  in the lower chromosphere. Two spectral features (lines in our case),
  observed simultaneously, significantly strengthen the constraints on
  a realistic model.

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Title: Magnetic field and radiative transfer modelling of a quiescent
    prominence
Authors: Gunár, S.; Schwartz, P.; Dudík, J.; Schmieder, B.; Heinzel,
   P.; Jurčák, J.
2014A&A...567A.123G    Altcode:
  <BR /> Aims: The aim of this work is to analyse the multi-instrument
  observations of the June 22, 2010 prominence to study its structure in
  detail, including the prominence-corona transition region and the dark
  bubble located below the prominence body. <BR /> Methods: We combined
  results of the 3D magnetic field modelling with 2D prominence fine
  structure radiative transfer models to fully exploit the available
  observations. <BR /> Results: The 3D linear force-free field model
  with the unsheared bipole reproduces the morphology of the analysed
  prominence reasonably well, thus providing useful information about
  its magnetic field configuration and the location of the magnetic
  dips. The 2D models of the prominence fine structures provide a good
  representation of the local plasma configuration in the region dominated
  by the quasi-vertical threads. However, the low observed Lyman-α
  central intensities and the morphology of the analysed prominence
  suggest that its upper central part is not directly illuminated from the
  solar surface. <BR /> Conclusions: This multi-disciplinary prominence
  study allows us to argue that a large part of the prominence-corona
  transition region plasma can be located inside the magnetic dips in
  small-scale features that surround the cool prominence material located
  in the dip centre. We also argue that the dark prominence bubbles
  can be formed because of perturbations of the prominence magnetic
  field by parasitic bipoles, causing them to be devoid of the magnetic
  dips. Magnetic dips, however, form thin layers that surround these
  bubbles, which might explain the occurrence of the cool prominence
  material in the lines of sight intersecting the prominence bubbles. <P
  />Movie and Appendix A are available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201322777/olm">http://www.aanda.org</A>

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Title: F-CHROMA.Flare Chromospheres: Observations, Models and Archives
Authors: Cauzzi, Gianna; Fletcher, Lyndsay; Mathioudakis, Mihalis;
   Carlsson, Mats; Heinzel, Petr; Berlicki, Arek; Zuccarello, Francesca
2014AAS...22412339C    Altcode:
  F-CHROMA is a collaborative project newly funded under the EU-Framework
  Programme 7 "FP7-SPACE-2013-1", involving seven different European
  research Institutes and Universities. The goal of F-CHROMA is to
  substantially advance our understanding of the physics of energy
  dissipation and radiation in the flaring solar atmosphere, with a
  particular focus on the flares' chromosphere. A major outcome of the
  F-CHROMA project will be the creation of an archive of chromospheric
  flare observations and models to be made available to the community
  for further research.In this poster we describe the structure and
  milestones of the project, the different activities planned, as well
  as early results. Emphasis will be given to the dissemination efforts
  of the project to make results of these activities available to and
  usable by the community.

---------------------------------------------------------
Title: On the formation of Mg ii h and k lines in solar prominences
Authors: Heinzel, P.; Vial, J. -C.; Anzer, U.
2014A&A...564A.132H    Altcode:
  <BR /> Aims: With the recent launch of the IRIS mission, it has become
  urgent to develop the spectral diagnostics using the Mg ii resonance
  h and k lines. In this paper, we aim to demonstrate the behavior of
  these lines under various prominence conditions. Our results serve
  as a basis for analysis of new IRIS data and for more sophisticated
  prominence modeling. <BR /> Methods: For this exploratory work,
  we use a canonical 1D prominence-slab model, which is isobaric
  and may have three different temperature structures: isothermal,
  PCTR-like (prominence-corona transition region), and consistent with
  the radiative equilibrium. The slabs are illuminated by a realistic
  incident solar radiation obtained from the UV observations. A five-level
  plus continuum Mg ii model atom is used to solve the full NLTE problem
  of the radiative transfer. We use the numerical code based on the ALI
  techniques and apply the partial frequency redistribution for both
  Mg ii resonance lines. We also use the velocity-dependent boundary
  conditions to study the effect of Doppler dimming in the case of
  moving prominences. Finally, the relaxation technique is used to
  compute a grid of models in radiative equilibrium. <BR /> Results:
  We computed the Mg ii h and k line profiles that are emergent from
  prominence-slab models and show their dependence on kinetic temperature,
  gas pressure, geometrical extension, and microturbulent velocity. By
  increasing the line opacity, significant departures from the complete
  frequency redistribution take place in the line wings. Models with a
  PCTR temperature structure show that Mg ii becomes ionized to Mg iii
  in the temperature range between roughly 15 000 and 30 000 K. Doppler
  dimming is significant for Mg ii resonance lines. At the velocity 300
  km s<SUP>-1</SUP>, the line intensity decreases to about 20% of the
  value for static prominences. Finally, we demonstrate the role of Mg
  ii h and k radiation losses on the prominence energy balance. Their
  dominant role is at lower pressures, while the losses due to hydrogen
  and Ca ii dominate at higher pressures.

---------------------------------------------------------
Title: Synthetic hydrogen spectra of prominence oscillations
Authors: Heinzel, P.; Zapiór, M.; Oliver, R.; Ballester, J. L.
2014A&A...562A.103H    Altcode: 2014arXiv1401.2131H
  Context. Prominence oscillations have been mostly detected using
  Doppler velocity, although there are also claimed detections by means
  of periodic variations in half-width or line intensity. However,
  scarce observational evidence exists about simultaneous detection of
  oscillations in several spectral indicators. <BR /> Aims: Our main aim
  here is to explore the relationship between spectral indicators, such
  as Doppler shift, line intensity, and line half-width, and the linear
  perturbations excited in a simple prominence model. <BR /> Methods:
  Our equilibrium background model consists of a bounded, homogeneous
  slab, which is permeated by a transverse magnetic field, having
  prominence-like physical properties. Assuming linear perturbations,
  the dispersion relation for fast and slow modes has been derived, as
  well as the perturbations for the different physical quantities. These
  perturbations have been used as the input variables in a one-dimensional
  radiative transfer code, which calculates the full spectral profile
  of the hydrogen Hα and Hβ lines. <BR /> Results: We have found that
  different oscillatory modes produce spectral indicator variations in
  different magnitudes. Detectable variations in the Doppler velocity
  were found for the fundamental slow mode only. Substantial variations
  in the Hβ line intensity were found for specific modes. Other modes
  lead to lower and even undetectable parameter variations. <BR />
  Conclusions: To perform prominence seismology, analysis of the Hα
  and Hβ spectral line parameters could be a good tool to detect and
  identify oscillatory modes.

---------------------------------------------------------
Title: A comparison between observed IRIS profiles of the h &amp;
    k doublet of Mg II and profiles from quiescent prominence NLTE models
Authors: Vial, Jean-Claude; Anzer, Ulrich; Heinzel, Petr; Kleint, Lucia
2014cosp...40E3515V    Altcode:
  With the advent of IRIS, it is now possible to investigate the cool core
  of prominences through the detailed profiles of the Mg II resonance
  lines with an unprecedented spatial resolution of 0.33 arcsecond. The
  slit-jaw camera also allows to record the temporal evolution of the
  prominence fine structure. We present IRIS observations of quiescent
  prominence profiles that we analyse in terms of reversal (if any),
  width, k/h line ratio, prominence/ quiet Sun line ratio. Comparing these
  parameters with the results of NLTE modelling (see Heinzel et al. 2014),
  we can derive thermodynamic parameters of the cool prominence plasma,
  along with the (line-of-sight) velocities and mass flows.

---------------------------------------------------------
Title: Possible measurements of the magnetic field in eruptive
    prominences using the PROBA-3 coronagraph
Authors: Serge, Koutchmy; Zhukov, Andrei; Dolla, Laurent; Heinzel,
   Petr; Lamy, Philippe; Bazin, Cyrille; Bommier, Veronique; Faurobert,
   Marianne
2014cosp...40E2971S    Altcode:
  The PROBA-3 mission will fly a spacecraft put in the shadow of a
  precisely occulting sister satellite orbiting “in formation” at a
  distance of 150 m in front of it to make artificial total eclipses. The
  region right above the solar limb will be studied for the first time
  over a coronal background not polluted by any spurious light. Although
  the priority will be the high-resolution fast imaging of the dynamic
  white-light corona, the use of a narrow filter centered on a low
  excitation D3 line of He I, is planned for imaging prominences. Adding
  the linear polarization analysis would permit the measurements of the
  magnetic field using the Hanle effect. We evaluate the possibility
  offered during the eruptive phase of a CME with prominence material
  inserted inside, for studying the associated magnetic field changes
  related to both the heating process and the ejection of material. The
  background highly polarized K-corona is taken into account. Sequences of
  quasi- simultaneous white-light processed images at high resolution are
  an additional feature of great interest for interpreting the overall
  magnetic structure.

---------------------------------------------------------
Title: A study of H I Lyman-alpha emission from prominences erupting
    in the intermediate corona and possible future applications for
    Solar Orbiter/METIS data
Authors: Bemporad, Alessandro; Heinzel, Petr; Jejcic, Sonja; Susino,
   Roberto
2014cosp...40E.273B    Altcode:
  Over almost the last 20 years hundreds of Coronal Mass Ejections
  (CME) have been observed by the UV Coronagraph Spectrometer (UVCS)
  onboard SOHO. For many of these events a significant emission in the HI
  Lyman-alpha lambda 1216 Å line was sampled during the transit across
  the slit of the erupting prominences embedded in the core of CMEs. The
  origin of this emission is completely different from what is typically
  observed by UVCS: because of the higher density and lower temperatures
  of such plasmas, the number of neutral H atoms is much larger than
  under typical coronal conditions, and the plasma is generally not
  optically thin at these wavelengths, as it is usually true for other
  coronal structures. Hence, the observed H I Lyman-alpha emission can be
  explained only if a radiative transport treatment across a moving plasma
  structure is considered. Once the proper boundary conditions are derived
  from the UV data, in combination with white light (WL) coronagraphic
  observations (from LASCO), we will show how the temperature and
  density of the erupting prominence could be derived even at large
  altitudes (typically larger than 0.6 solar radii above the limb),
  thus providing information on heating/cooling and ionization of the
  CME core during the eruption. These results are very important in the
  light of coronagraphic observations that will be provided by the METIS
  instrument onboard the Solar Orbiter: because METIS will contemporary
  observe the solar corona in WL and in UV (HI Lyman-alpha), it will be
  possible to derive, with a technique similar to what is shown here,
  very important information on prominence plasmas embedded in the core
  of CMEs and crossing the METIS instrument field of view.

---------------------------------------------------------
Title: Chromospheric heating during a flare
Authors: Heinzel, Petr
2014cosp...40E1183H    Altcode:
  Flares are now believed to be complex processes initiated in the corona
  and largely influencing the lower atmospheric layers. The energy
  is transported from the corona down to the chromosphere and even
  photosphere in various modes and this leads to significant heating
  of the chromospheric plasma. We will review individual processes
  among which the most important is the particle-beam propagation and
  dissipation, but others as conduction, XUV heating, wave heating
  etc. are also to be considered. We will summarize recent results of
  the radiation-hydrodynamical simulations of the chromospheric heating
  during flares and the progress in our understanding of the basic
  heating mechanisms and flows. We will also point to new space and
  ground observations which provide the critical constraints to modeling.

---------------------------------------------------------
Title: Mapping prominence plasma parameters from eclipse observations
Authors: Jejčič, Sonja; Heinzel, Petr; Zapiór, Maciej; Druckmüller,
   Miloslav; Gunár, Stanislav; Kotrč, Pavel
2014IAUS..300..420J    Altcode:
  Using the eclipse observations, we construct the maps of quiescent
  prominence temperatures, electron densities, pressures and geometrical
  thicknesses. For this we use the RGB signal of prominence visible-light
  emission detected during the total solar eclipse on August 1, 2008
  in Mongolia, and quasi-simultaneous Hα spectra taken at Ondřejov
  observatory. The method of disentangling the electron density and
  effective geometrical thickness was described by Jejčič &amp;
  Heinzel (2009) and is used here for the first time to analyse the
  spatial variations of various prominence parameters.

---------------------------------------------------------
Title: An Estimate of Chromospheric Heating by Acoustic Waves
Authors: Sobotka, M.; Švanda, M.; Jurčak, J.; Heinzel, P.; Del Moro,
   D.; Berrilli, F.
2014CEAB...38...53S    Altcode:
  Several mechanisms may heat the solar chromosphere: acoustic waves,
  magnetoacoustic waves (slow, fast, and Alfvén waves), and small-scale
  magnetic reconnections. Based on observations in the Ca II 854.2 nm
  line, the contribution of acoustic waves to the heating of quiet and
  plage regions in the chromosphere is discussed. The energy released
  by radiative losses is compared with the energy deposited by acoustic
  waves. Radiative losses are computed using a grid of six semi-empirical
  models VAL A--F. The deposited acoustic flux is calculated using power
  spectra of Doppler oscillations measured in the Ca~II line core. The
  comparison shows that the spatial correlation of maps of radiative
  losses and acoustic flux is 70 %. The deposited acoustic flux provides
  at least 25--30~% of the energy radiated in the quiet chromosphere
  and 50~% in plage regions.

---------------------------------------------------------
Title: Non-LTE Modeling and Observations of Oscillating Prominences
Authors: Zapiór, M.; Heinzel, P.; Oliver, R.; Ballester, J. L.;
   Kotrč, P.
2014IAUS..300...52Z    Altcode:
  Prominence oscillations have been mostly detected using Doppler
  velocity, although there are also claimed detections by means of the
  periodic variations of half-width or line intensity. Our main aim
  here is to explore the relationship between spectral indicators such
  as Doppler shift, line intensity and line half-width and the linear
  perturbations excited in a simple prominence model.

---------------------------------------------------------
Title: Kappa-distributions and Temperature Structure of the
    Prominence-Corona Transition Region
Authors: Dzifčáková, Elena; Mackovjak, Šimon; Heinzel, Petr
2014IAUS..300..408D    Altcode:
  The influence of the electron κ - distributions on the differential
  emission measure (DEM) of the prominence-corona transition region
  (PCTR) derived from observed line intensities has been investigated. An
  important consequence of the κ - distribution is formation of the
  emission lines in much wider temperature ranges. The implications
  for the formation temperature of the observed SDO/AIA band emissions
  are shown.

---------------------------------------------------------
Title: MgII lines in solar flares: IRIS observations and NLTE modeling
Authors: Heinzel, Petr; Kasparova, Jana; Kleint, Lucia; Dzifcakova,
   Elena
2014cosp...40E1182H    Altcode:
  Chromospheric flares have been recently observed in MgII resonance
  lines by the IRIS instrument. Apart from the resonance lines h and k,
  also subordinate line emissions due to transitions between the MgII
  levels 3P and 3D have been now detected by IRIS during flares. We apply
  the NLTE radiative-transfer code to synthesize all these MgII lines
  under typical flare conditions. In particular, we focus on the role
  of the non-thermal excitations and ionizations, which are due to the
  presence of the electron beams and corresponding return currents. The
  results of this modeling are compared with new IRIS data.

---------------------------------------------------------
Title: Dynamics of the solar atmosphere above a pore with a light
    bridge
Authors: Sobotka, M.; Švanda, M.; Jurčák, J.; Heinzel, P.; Del Moro,
   D.; Berrilli, F.
2013A&A...560A..84S    Altcode: 2013arXiv1309.7790S
  Context. Solar pores are small sunspots lacking a penumbra that have
  a prevailing vertical magnetic-field component. They can include light
  bridges at places with locally reduced magnetic field. Like sunspots,
  they exhibit a wide range of oscillatory phenomena. <BR /> Aims:
  A large isolated pore with a light bridge (NOAA 11005) is studied
  to obtain characteristics of a chromospheric filamentary structure
  around the pore, to analyse oscillations and waves in and around
  the pore, and to understand the structure and brightness of the light
  bridge. <BR /> Methods: Spectral imaging observations in the line Ca II
  854.2 nm and complementary spectropolarimetry in Fe I lines, obtained
  with the DST/IBIS spectrometer and HINODE/SOT spectropolarimeter,
  were used to measure photospheric and chromospheric velocity fields,
  oscillations, waves, the magnetic field in the photosphere, and
  acoustic energy flux and radiative losses in the chromosphere. <BR />
  Results: The chromospheric filamentary structure around the pore has
  all important characteristics of a superpenumbra: it shows an inverse
  Evershed effect and running waves, and has a similar morphology and
  oscillation character. The granular structure of the light bridge in
  the upper photosphere can be explained by radiative heating. Acoustic
  waves leaking up from the photosphere along the inclined magnetic
  field in the light bridge transfer enough energy flux to balance
  the entire radiative losses of the light-bridge chromosphere. <BR />
  Conclusions: A penumbra is not a necessary condition for the formation
  of a superpenumbra. The light bridge is heated by radiation in the
  photosphere and by acoustic waves in the chromosphere.

---------------------------------------------------------
Title: Scattering Polarization in Solar Flares
Authors: Štěpán, Jiří; Heinzel, Petr
2013ApJ...778L...6S    Altcode: 2013arXiv1310.3284S
  There is ongoing debate about the origin and even the very existence
  of a high degree of linear polarization of some chromospheric
  spectral lines observed in solar flares. The standard explanation
  of these measurements is in terms of the impact polarization caused
  by non-thermal proton and/or electron beams. In this work, we study
  the possible role of resonance line polarization due to radiation
  anisotropy in the inhomogeneous medium of the flare ribbons. We
  consider a simple two-dimensional model of the flaring chromosphere
  and we self-consistently solve the non-LTE problem taking into
  account the role of resonant scattering polarization and of the
  Hanle effect. Our calculations show that the horizontal plasma
  inhomogeneities at the boundary of the flare ribbons can lead to a
  significant radiation anisotropy in the line formation region and,
  consequently, to a fractional linear polarization of the emergent
  radiation of the order of several percent. Neglecting the effects of
  impact polarization, our model can provide a clue for resolving some
  of the common observational findings, namely: (1) why a high degree
  of polarization appears mainly at the edges of the flare ribbons;
  (2) why polarization can also be observed during the gradual phase of
  a flare; and (3) why polarization is mostly radial or tangential. We
  conclude that radiation transfer in realistic multi-dimensional models
  of solar flares needs to be considered as an essential ingredient for
  understanding the observed spectral line polarization.

---------------------------------------------------------
Title: Atmosphere above a large solar pore
Authors: Sobotka, M.; Švanda, M.; Jurčák, J.; Heinzel, P.; Del
   Moro, D.
2013JPhCS.440a2049S    Altcode: 2013arXiv1302.4893S
  A large solar pore with a granular light bridge was observed on October
  15, 2008 with the IBIS spectrometer at the Dunn Solar Telescope and a
  69-min long time series of spectral scans in the lines Ca II 854.2 nm
  and Fe I 617.3 nm was obtained. The intensity and Doppler signals in the
  Ca II line were separated. This line samples the middle chromosphere
  in the core and the middle photosphere in the wings. Although no
  indication of a penumbra is seen in the photosphere, an extended
  filamentary structure, both in intensity and Doppler signals, is
  observed in the Ca II line core. An analysis of morphological and
  dynamical properties of the structure shows a close similarity to a
  superpenumbra of a sunspot with developed penumbra. A special attention
  is paid to the light bridge, which is the brightest feature in the
  pore seen in the Ca II line centre and shows an enhanced power of
  chromospheric oscillations at 3-5 mHz. Although the acoustic power
  flux in the light bridge is five times higher than in the "quiet"
  chromosphere, it cannot explain the observed brightness.

---------------------------------------------------------
Title: Puzzling nature of the fine structure of quiescent prominences
    and filaments
Authors: Gunár, Stanislav; Heinzel, Petr; Anzer, Ulrich; Mackay,
   Duncan H.
2013JPhCS.440a2035G    Altcode:
  Even after more than 160 years of observations and modelling of solar
  prominences their true nature contains many open questions. In this
  work we argue that current 2D prominence fine structure models can
  help us to understand the puzzling connection between quasi-vertical
  fine structures often seen in quiescent prominences observed on the
  solar limb and horizontally aligned dark fibrils representing the fine
  structures of prominences observed in absorption against the solar disk
  (filaments).

---------------------------------------------------------
Title: Observations and Modeling of Stellar Flares
Authors: Heinzel, P.
2013POBeo..92...87H    Altcode:
  We briefly review the current status of observations of stellar flares
  with meter-class telescopes and their relation to observations of flares
  on the Sun-as-a-star. Both stellar photometry and spectroscopy will
  be discussed. Solar and stellar flares are modeled using the methods
  of radiation hydrodynamics and we will make a summary of recent results.

---------------------------------------------------------
Title: Non-linear force-free magnetic dip models of quiescent
    prominence fine structures
Authors: Gunár, S.; Mackay, D. H.; Anzer, U.; Heinzel, P.
2013A&A...551A...3G    Altcode:
  <BR /> Aims: We use 3D non-linear force-free magnetic field modeling
  of prominence/filament magnetic fields to develop the first 2D models
  of individual prominence fine structures based on the 3D configuration
  of the magnetic field of the whole prominence. <BR /> Methods: We use
  an iterative technique to fill the magnetic dips produced by the 3D
  modeling with realistic prominence plasma in hydrostatic equilibrium
  and with a temperature structure that contains the prominence-corona
  transition region. With this well-defined plasma structure the radiative
  transfer can be treated in detail in 2D and the resulting synthetic
  emission can be compared with prominence/filament observations. <BR
  /> Results: Newly developed non-linear force-free magnetic dip models
  are able to produce synthetic hydrogen Lyman spectra in a qualitative
  agreement with a range of quiescent prominence observations. Moreover,
  the plasma structure of these models agrees with the gravity induced
  prominence fine structure models which have already been shown to
  produce synthetic spectra in good qualitative agreement with several
  observed prominences. <BR /> Conclusions: We describe in detail the
  iterative technique which can be used to produce realistic plasma
  models of prominence fine structures located in prominence magnetic
  field configurations containing dips, obtained using any kind of
  magnetic field modeling.

---------------------------------------------------------
Title: SDO/AIA Prominence physical conditions
Authors: Schmieder, B.; Parenti, S.; Dudik, J.; Aulanier, G.; Heinzel,
   P.; Zapior, M.; Golub, L.
2013enss.confE..27S    Altcode:
  SDO/AIA has carried out continuous observations of prominences in
  multiple wavelengths, with high spatial and temporal resolution. These
  data provide us an opportunity to understand the physical conditions
  and dynamics of prominences. The surprising brightness of prominences
  in some coronal lines has been well explained by the presence of
  transition region lines in the bandpass of the filters (171 A, 131 A),
  a result that leads us to revise our model of the transition region
  of prominences and to consider a relatively dense transition region in
  some prominence evolutionary phases or in some viewing orientation. An
  additional aspect of prominence dynamics will be presented with a new
  quasi-static MHD model proposed for bubbles and plumes. We propose
  an alternative to the interpretation that thermal instabilities are
  responsible for the formation of bubbles. The bubbles are found to
  correspond to magnetic separatrices formed by emerging magnetic field
  close to prominence footpoints.

---------------------------------------------------------
Title: Magnetic Topology of Bubbles in Quiescent Prominences
Authors: Dudík, J.; Aulanier, G.; Schmieder, B.; Zapiór, M.;
   Heinzel, P.
2012ApJ...761....9D    Altcode:
  We study a polar-crown prominence with a bubble and its plume observed
  in several coronal filters by the SDO/AIA and in Hα by the MSDP
  spectrograph in Białków (Poland) to address the following questions:
  what is the brightness of prominence bubbles in EUV with respect to the
  corona outside of the prominence and the prominence coronal cavity? What
  is the geometry and topology of the magnetic field in the bubble? What
  is the nature of the vertical threads seen within prominences? We
  find that the brightness of the bubble and plume is lower than the
  brightness of the corona outside of the prominence, and is similar to
  that of the coronal cavity. We constructed linear force-free models of
  prominences with bubbles, where the flux rope is perturbed by inclusion
  of parasitic bipoles. The arcade field lines of the bipole create the
  bubble, which is thus devoid of magnetic dips. Shearing the bipole or
  adding a second one can lead to cusp-shaped prominences with bubbles
  similar to the observed ones. The bubbles have complex magnetic
  topology, with a pair of coronal magnetic null points linked by a
  separator outlining the boundary between the bubble and the prominence
  body. We conjecture that plume formation involves magnetic reconnection
  at the separator. Depending on the viewing angle, the prominence can
  appear either anvil-shaped with predominantly horizontal structures,
  or cusp-shaped with predominantly vertical structuring. The latter
  is an artifact of the alignment of magnetic dips with respect to the
  prominence axis and the line of sight.

---------------------------------------------------------
Title: Magnetism of Solar Flares and Prominences
Authors: Heinzel, P.; Hudson, H. S.
2012ASPC..463..121H    Altcode:
  We give an overview of magnetic fields in solar flares and
  prominences. Magnetic fields related to flares play a crucial role in
  the process of energy release and transport to the lower atmosphere,
  and thus magnetometry under the coronal and chromospheric conditions is
  extremely challenging. Magnetic fields in prominences are supposed to
  keep the prominence plasma at coronal heights against the gravity. Their
  measurements have been numerous, but high-resolution mapping is still
  missing. We discuss various flare and prominence models in connection
  to current and future high-resolution observations.

---------------------------------------------------------
Title: Study of an Extended EUV Filament Using SoHO/SUMER Observations
    of the Hydrogen Lyman Lines. II. Lyman α Line Observed During a
    Multi-wavelength Campaign
Authors: Schwartz, P.; Schmieder, B.; Heinzel, P.; Kotrč, P.
2012SoPh..281..707S    Altcode: 2012SoPh..tmp..201S
  A filament and its channel close to the solar disk were observed in the
  complete hydrogen Lyman spectrum, and in several EUV lines by the SUMER
  (Solar Ultraviolet Measurement of Emitted Radiation) and CDS (Coronal
  Diagnostic Spectrometer) spectrographs on the SoHO satellite, and in
  Hα by ground-based telescopes during a multi-instrument campaign in
  May 2005. It was a good opportunity to get an overview of the volume
  and the density of the cold plasma in the filament channel; these are
  essential parameters for coronal mass ejections. We found that the
  width of the filament depends on the wavelength in which the filament
  is observed (around 15 arcsec in Hα, 30 arcsec in Lα, and 60 arcsec
  in EUV). In Lα the filament is wider than in Hα because cool plasma,
  not visible in Hα, is optically thick at the Lα line center, and its
  presence blocks the coronal emission. We have derived physical plasma
  properties of this filament fitting the Lyman spectra and Hα profiles
  by using a 1D isobaric NLTE model. The vertical temperature profile
  of the filament slab is flat (T≈7000 K) with an increase to ≈ 20
  000 K at the top and the bottom of the slab. From an analysis of the
  Lα and Hα source functions we have concluded that these lines are
  formed over the whole filament slab. We have estimated the geometrical
  filling factor in the filament channel. Its low value indicates the
  presence of multi-threads.

---------------------------------------------------------
Title: Formation of Balmer Lines in Impulsively Heated Flare
    Atmosphere by Neutral Beams
Authors: Varady, M.; Kašparová, J.; Moravec, Z.; Karlický, M.;
   Heinzel, P.
2012ASPC..454..341V    Altcode:
  In the context of interpreting non-thermal hard X-ray emission and γ
  lines emanating from the footpoints of flare loops, most contemporary
  flare models assign a fundamental role during the flare energy release,
  transport and deposition to the high energy non-thermal particle
  beams. In this contribution we concentrate on modelling of the
  spectroscopic properties of chromospheric flare emission in optical
  hydrogen lines generated due to the bombardment of the chromosphere
  and photosphere by neutral beams with power-law spectra. In order
  to obtain an estimate of the neutral beam flare heating in the solar
  atmosphere we produced a simple model describing the propagation and
  thermalisation of neutral beams. We compare the neutral beam flare
  heating with the flare heating produced by corresponding pure electron
  and proton beams. Further we compare the contribution functions for
  Hα line obtained for neutral and electron beam heating.

---------------------------------------------------------
Title: Velocity Vector, Ionization Degree, and Temperature of
    Prominence Fine Structures Observed by Hinode/SOT
Authors: Schmieder, B.; Mein, P.; Chandra, R.; Molodij, G.; Heinzel,
   P.; Berlicki, A.; Schwartz, P.; Fárník, F.; Labrosse, N.; Anzer,
   U.; Watanabe, T.
2012ASPC..454..107S    Altcode:
  Prominences have been successfully observed by Hinode in April 2007
  exhibiting a strong dynamics of their fine structures. The dynamics
  of a prominence is a challenge to understand the formation of cool
  prominence plasma embedded in the hot corona. Combining simultaneous
  observations obtained in Hα with Hinode/SOT and the MSDP spectrograph
  operating at the Meudon solar tower, velocity vectors have been
  derived. The Doppler-shifts of bright threads are of the same order
  as the velocities measured perpendicular to the line of sight. This
  suggests that the vertical structures of the prominence could be a pile
  up of dips in magnetic field lines viewed in 3D. Using Hα, Hinode/XRT
  and TRACE data, the hydrogen ionization degree has been determined to
  be 0.5-0.8, and the optical thickness in Hα between 0.2 and 1.3. The
  Extreme Ultraviolet Imaging Spectrometer (EIS) on Hinode produced images
  of the prominence in 11 selected lines with formation temperatures
  between log(T) = 4.7 and log(T) = 6.1. We comment on the absorption,
  emissivity blocking and emission involved for interpreting the different
  structures of the prominence in terms of the temperature and density.

---------------------------------------------------------
Title: Mass of Solar Prominences Estimated from Multi-Wavelength Data
Authors: Schwartz, P.; Fárník, F.; Heinzel, P.; Kotrč, P.; Anzer, U.
2012ASPC..454..117S    Altcode:
  The mass of selected prominences was estimated using their
  multi-wavelength observations: in Hα by the HSFA2 spectrograph of
  the Ondřejov observatory, in EUV by SoHO/EIT and in the soft X-rays
  by Hinode XRT. The results are compared with values estimated by
  other authors.

---------------------------------------------------------
Title: Prominences observations with SDO/AIA
Authors: Parenti, Susanna; Schmieder, Brigitte; Golub, Leon; Heinzel,
   Petr
2012cosp...39.1447P    Altcode: 2012cosp.meet.1447P
  The Prominence-Corona-Transition-Region (PCTR) plays a key role in
  the thermal and pressure equilibrium of prominences. However, several
  open issues limit our knowledge of this important interface. Among
  them we find the thermal structure and the maximum temperature of
  its emitting plasma. This work is a new step toward resolving these
  issues. By noting that prominences may be observed in emission in
  the 171 and 131 SDO/AIA images, while they are seen in absorption in
  others (e.g. 193) we investigate the temperature content of these
  channels. Using the CHIANTI atomic database and previously derived
  prominence DEMs, we built synthetic spectra in these AIA channels to
  establish the main contributors. We find that the Fe IX line always
  dominates the 171 band, even in absence of a coronal plasma, while
  the 131 channel is dominated by Fe VIII. Our conclusion is that the
  PCTR reaches, at least, 4x 10^5 K.

---------------------------------------------------------
Title: On the Nature of Prominence Emission Observed by SDO/AIA
Authors: Parenti, S.; Schmieder, B.; Heinzel, P.; Golub, L.
2012ApJ...754...66P    Altcode: 2012arXiv1205.5460P
  The prominence-corona transition region (PCTR) plays a key role in the
  thermal and pressure equilibrium of solar prominences. Our knowledge
  of this interface is limited and several major issues remain open,
  including the thermal structure and, in particular, the maximum
  temperature of the detectable plasma. The high signal-to-noise
  ratio of images obtained by the Atmospheric Imaging Assembly (AIA)
  on NASA's Solar Dynamics Observatory clearly shows that prominences
  are often seen in emission in the 171 and 131 bands. We investigate the
  temperature sensitivity of these AIA bands for prominence observations,
  in order to infer the temperature content in an effort to explain the
  emission. Using the CHIANTI atomic database and previously determined
  prominence differential emission measure distributions, we build
  synthetic spectra to establish the main emission-line contributors
  in the AIA bands. We find that the Fe IX line always dominates
  the 171 band, even in the absence of plasma at &gt;10<SUP>6</SUP> K
  temperatures, while the 131 band is dominated by Fe VIII. We conclude
  that the PCTR has sufficient plasma emitting at &gt;4 × 10<SUP>5</SUP>
  K to be detected by AIA.

---------------------------------------------------------
Title: Dynamics of quiescent prominences
Authors: Heinzel, Petr
2012cosp...39..742H    Altcode: 2012cosp.meet..742H
  We review the state-of-the-art of the observations and modeling of
  prominence fine structures, with special emphasis on the dynamics. Fine
  structures of quiescent prominences have been recently observed by
  Hinode/SOT and these observations revealed a rather complex dynamics
  of bright threads and blobs and of dark plumes originating from large
  prominence bubbles. SOHO/SUMER spectra of hydrogen Lyman lines, together
  with H-alpha observations from MSDP, provide us with constraints on
  the dynamics of cool fine structures. 2D non-LTE modeling is used for
  analysis of the line profiles and their asymmetries. On the contrary,
  the SDO/AIA images, together with RHD modeling of dipped magnetic loops,
  lead to a better understanding of the dynamics and energetics of hotter
  prominence plasmas. Finally, some more global dynamics is revealed by
  the spectroscopic detection of quiescent prominence oscillations. We
  show recent results of such observations and new radiative-transfer
  modeling.

---------------------------------------------------------
Title: Can bubbles in quiescent prominences be purely magnetic
    phenomena?
Authors: Dudik, Jaroslav; Schmieder, Brigitte; Aulanier, Guillaume;
   Zapior, Maciej; Heinzel, Petr
2012cosp...39..486D    Altcode: 2012cosp.meet..486D
  We present a model of the magnetic field constituting quiescent
  prominences. The model assumes a linear force-free field with a
  weakly twisted flux-tube in an OX/OF topology perturbed by presence
  of parasitic polarities within the filament channel. The parasitic
  polarities locally create the cusp-shaped prominences with bubbles
  exactly as those observed by the SDO/AIA and Bialkow Observatory. We
  find that the observations are best reproduced if the parasitic bipoles
  are sheared with respect to the main inversion line. We show that
  the bubbles are in fact constituted by the arcade-like field lines,
  as opposed to that of the prominence, which is created by magnetic
  dips. A pair of null points is always associated with the parasitic
  bipole. These null points are connected by a separator passing through
  the prominence bubble. We show how the presence of an additional
  parasitic bipole moves the separator to the boundary between the bubble
  and the rest of the prominence, producing a topology favorable for
  reconnection and possibly for the formation of plumes.

---------------------------------------------------------
Title: Prominence fine-structure dynamics as inferred from 2D
    non-LTE models
Authors: Gunar, Stanislav; Schmieder, Brigitte; Mein, Pierre;
   Heinzel, Petr
2012cosp...39..683G    Altcode: 2012cosp.meet..683G
  2D multi-thread prominence fine structure models are able to
  produce synthetic Lyman spectra in very good agreement with spectral
  observations by SOHO/SUMER including the spectral line asymmetries. The
  synthetic differential emission measure curves derived from these
  models are also in a good agreement with observations. Now we show that
  these models are also able to produce synthetic H-alpha line profiles
  in very good agreement with observations which allows us to analyze
  not only the physical parameters of the prominence fine-structure
  plasma but also some aspects of its dynamical behaviour. We compare
  the synthetic H-alpha spectra with the observed spectra of the
  April 26, 2007 prominence using three statistical parameters: the
  line integrated intensity, the line full-width at the half-maximum
  (FWHM), and the Doppler velocity derived from shifts of the line
  profiles. This statistical analysis allows us to conclude that the
  overall statistical distribution of the LOS velocities in the April 26,
  2007 prominence at the time of the observations was below +/-15 km/s
  and in the prominence core was close to +/-10 km/s. In combination
  with the analysis of the Lyman spectra we determine several physical
  parameters of the observed prominence fine structures which show that
  the April 26, 2007 prominence was relatively less massive. We are also
  able to put some constrains on the prominence core temperature that
  might be relatively low, reaching values below 6000 K.

---------------------------------------------------------
Title: SDO/EVE spectra of solar flares
Authors: Heinzel, Petr; Avrett, Eugene; Dzifcakova, Elena; Hudson,
   Hugh S.
2012cosp...39..743H    Altcode: 2012cosp.meet..743H
  For selected flare events we present the SDO/EVE spectra of hydrogen
  and helium resonance continua and compare them with the results of
  non-LTE transfer computations based on various flare models. We
  discuss the formation of these continua and their diagnostic
  potential for determination of the temperature structure of the
  flaring atmosphere. Under the optically-thin conditions, we synthesize
  these resonance continua using the CHIANTI database where we added
  the relevant non-thermal atomic rates. This shows how the electron
  or proton beams may affect the continua during an impulsive phase of
  solar flares. As a benchmark we present our comparison of the quiet-Sun
  EVE spectra with the flux synthesized from the model C6 of Avrett and
  Loeser (2008). Our study has a more general relevance to the physics
  of stellar flares.

---------------------------------------------------------
Title: Dynamics of quiescent prominence fine structures analyzed by
    2D non-LTE modelling of the Hα line
Authors: Gunár, S.; Mein, P.; Schmieder, B.; Heinzel, P.; Mein, N.
2012A&A...543A..93G    Altcode:
  <BR /> Aims: We analyze the dynamics of the prominence fine
  structures of a quiescent prominence observed on April 26, 2007
  during a coordinated campaign of several spaceborne and ground-based
  instruments. We use Lyman spectra observed by SOHO/SUMER and the
  Hα line spectra obtained by MSDP spectrograph working at the
  Meudon Solar Tower. <BR /> Methods: We employ the 2D multi-thread
  prominence fine-structure modelling that includes randomly distributed
  line-of-sight (LOS) velocities of individual threads to derive models
  producing synthetic Lyman lines in good agreement with the SOHO/SUMER
  observations. We then use these models to produce synthetic Hα
  line spectra that we compare with the observed spectra using three
  statistical parameters: the line integrated intensity, the line
  full-width at half-maximum (FWHM), and the Doppler velocity derived
  from shifts of the line profiles. <BR /> Results: We demonstrate that
  the 2D multi-thread models that produce synthetic Lyman spectra in
  agreement with observations also generate synthetic Hα spectra in
  good agreement with the observed ones. The statistical analysis of the
  FWHM and Doppler velocities of the synthetic Hα line profiles show
  that the overall LOS velocities in the April 26, 2007 prominence at
  the time of the observations were below 15 km s<SUP>-1</SUP> and in
  the prominence core were close to 10 km s<SUP>-1</SUP>. In combination
  with the analysis of the Lyman spectra, we determine several physical
  parameters of the observed prominence fine-structures that show
  that the April 26, 2007 prominence had a relatively low-mass weakly
  magnetized structure. We are also able to impose some constraints
  on the prominence core temperature, which may be relatively low,
  with values below 6000 K. <BR /> Conclusions: The combination of
  2D non-LTE prominence fine-structure modelling with the statistical
  analysis of the observed and synthetic Lyman and Hα spectra allows us
  to analyze the influence of the model input parameters and the velocity
  fields on the synthetic Hα line profiles, thus determine the overall
  dynamics of the observed prominence as well as the physical parameters
  of its plasma. <P />Appendix A is available in electronic form at <A
  href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: On the Visibility of Solar Prominences in SDO/AIA Channels
Authors: Heinzel, P.; Schmieder, B.; Parenti, S.; Golub, L.
2012ASPC..456...75H    Altcode:
  Prominences in EUV lines are observed as dark structures over the
  limb due absorption and emission blocking mechanisms. However, at 171
  Å is observed emission in prominences with TRACE and SDO/AIA, and
  it is believed to be due to the prominence-corona transition region
  (PCTR) emitting in cool lines. To check this, we use the Differential
  Emission Measure (DEM) recently obtained for quiescent prominences
  using SOHO/SUMER spectra (Parenti and Vial 2007) and compute the
  synthetic spectra in selected AIA channels. We then compare 171 Å and
  195 Å channels and derive conclusions concerning the PCTR emissivity,
  as well well as the absorption and blocking. The emission seen in the
  171 Å channel can be used to better constrain prominence DEM curves.

---------------------------------------------------------
Title: On the Nature of Prominence Bubbles and Plumes
Authors: Schmieder, B.; Zapior, M.; Heinzel, P.; Aulanier, G.
2012ASPC..456...77S    Altcode:
  An example of bubble and related plume, using time series in
  selected SDO/AIA channels and co-temporal MSDP observations in the
  Hα line obtained at Wroclaw-Bialkow observatory on April 20, 2011 is
  presented. The formation of bubbles may be due to emerging arcades in
  the filament channel, below the prominence. After discussing on MHD
  modeling, we conclude that bubbles and plumes are parts of the corona
  observed through gaps/windows in the prominence.

---------------------------------------------------------
Title: Optical-to-Radio Continua in Solar Flares
Authors: Heinzel, P.; Avrett, E. H.
2012SoPh..277...31H    Altcode:
  Spectral continua observed during solar flares may contain information
  about both thermal and non-thermal heating mechanisms. Using two
  semi-empirical flare models F2 and FLA, we synthesize the thermal
  continua from optical to mm-radio domains and compare their intensities
  with quiet-Sun values computed from a recent model C7. In this
  way, the far-infrared and sub-mm/mm continua are studied for the
  first time, and we present our results as a benchmark for further
  modeling and for planning new observations, especially with the ALMA
  instrument. Finally, we demonstrate how these continua are formed and
  show a close correspondence between their brightness temperature and
  the kinetic-temperature structure of the flaring atmosphere.

---------------------------------------------------------
Title: Radiative equilibrium in solar prominences reconsidered
Authors: Heinzel, P.; Anzer, U.
2012A&A...539A..49H    Altcode:
  <BR /> Aims: We reconsider the question which kinetic temperatures
  can lead to prominence configurations that are in radiative
  equilibrium. We compare these temperatures to those from other
  calculations. <BR /> Methods: For this purpose we solved the full
  non-LTE radiative-transfer problem for a gas consisting of hydrogen,
  helium and calcium. We used simple isobaric 1D slabs and began with
  isothermal models. Then we solved the radiative-relaxation problem
  and determined the radiative-equilibrium conditions within the
  whole slab. <BR /> Results: By adding the calcium radiative losses,
  we found that these equilibrium temperatures are considerably lower
  than those obtained for a pure hydrogen gas. This is because the newly
  calculated CaII line losses appear to play a significant role in the
  energy balance, similar to chromospheric conditions. The equilibrium
  temperatures obtained span the range between 4400-9500 K, depending
  on the gas pressure and slab thickness.

---------------------------------------------------------
Title: The nature of hydrogen and helium continua in SDO/EVE spectra
    of solar flares
Authors: Heinzel, P.; Avrett, E. H.
2012decs.confE.109H    Altcode:
  For selected flare events we present the SDO/EVE spectra of hydrogen
  and helium resonance continua and compare them with the results
  of the non-LTE transfer computations based on semi-empirical flare
  models. We discuss the formation of these continua and their diagnostic
  potential for determination of the temperature structure of the flaring
  atmosphere. Non-thermal processes are also considered. As a benchmark
  we present our comparison of the quiet-Sun EVE spectra with the flux
  synthesized from the model C6 of Avrett and Loeser (2008).

---------------------------------------------------------
Title: Formation of MgII lines in solar prominences
Authors: Heinzel, Petr
2012decs.confE.108H    Altcode:
  Solar prominences have been observed in MgII h and k lines, both from
  space (OSO-8) or from stratospheric balloons. Non-LTE modeling of these
  resonance lines was then performed and the results have been compared
  to available observations. We briefly review this past effort and
  present new transfer computations which take into account all details
  of the MgII line formation under realistic prominence conditions. We
  estimate the role of MgII lines in radiation cooling of prominence
  plasmas and show how they affect the radiative relaxation in these
  structures. Finally, we also demonstrate the diagnostic capabilities
  of these lines useful for thermodynamic and velocity measurements.

---------------------------------------------------------
Title: Splinter Session "Solar and Stellar Flares"
Authors: Fletcher, L.; Hudson, H.; Cauzzi, G.; Getman, K. V.; Giampapa,
   M.; Hawley, S. L.; Heinzel, P.; Johnstone, C.; Kowalski, A. F.; Osten,
   R. A.; Pye, J.
2011ASPC..448..441F    Altcode: 2011csss...16..441F; 2012arXiv1206.3997F
  This summary reports on papers presented at the Cool Stars-16 meeting in
  the splinter session "Solar and Stellar flares." Although many topics
  were discussed, the main themes were the commonality of interests,
  and of physics, between the solar and stellar flare communities,
  and the opportunities for important new observations in the near future.

---------------------------------------------------------
Title: Synthetic differential emission measure curves of prominence
    fine structures. II. The SoHO/SUMER prominence of 8 June 2004
Authors: Gunár, S.; Parenti, S.; Anzer, U.; Heinzel, P.; Vial, J. -C.
2011A&A...535A.122G    Altcode:
  <BR /> Aims: This study is the first attempt to combine the prominence
  observations in Lyman, UV, and EUV lines with the determination of the
  prominence differential emission measure derived using two different
  techniques, one based on the inversion of the observed UV and EUV lines
  and the other employing 2D non-LTE prominence fine-structure modeling
  of the Lyman spectra. <BR /> Methods: We use a trial-and-error method
  to derive the 2D multi-thread prominence fine-structure model producing
  synthetic Lyman spectra in good agreement with the observations. We then
  employ a numerical method to perform the forward determination of the
  DEM from 2D multi-thread models and compare the synthetic DEM curves
  with those derived from observations using inversion techniques. <BR
  /> Results: A set of available observations of the June 8, 2004
  prominence allows us to determine the range of input parameters, which
  contains models producing synthetic Lyman spectra in good agreement
  with the observations. We select three models, which represent this
  parametric-space area well and compute the synthetic DEM curves for
  multi-thread realizations of these models. The synthetic DEM curves
  of selected models are in good agreement with the DEM curves derived
  from the observations. <BR /> Conclusions: We show that the evaluation
  of the prominence fine-structure DEM complements the analysis of the
  prominence hydrogen Lyman spectra and that its combination with the
  detailed radiative-transfer modeling of prominence fine structures
  provides a useful tool for investigating the prominence temperature
  structure from the cool core to the prominence-corona transition region.

---------------------------------------------------------
Title: EUV lines observed with EIS/Hinode in a solar prominence
Authors: Labrosse, N.; Schmieder, B.; Heinzel, P.; Watanabe, T.
2011A&A...531A..69L    Altcode: 2011arXiv1105.1400L
  Context. During a multi-wavelength observation campaign with Hinode
  and ground-based instruments, a solar prominence was observed for
  three consecutive days as it crossed the western limb of the Sun
  in April 2007. <BR /> Aims: We report on observations obtained on
  26 April 2007 using EIS (Extreme ultraviolet Imaging Spectrometer)
  on Hinode. They are analysed to provide a qualitative diagnostic
  of the plasma in different parts of the prominence. <BR /> Methods:
  After correcting for instrumental effects, the rasters at different
  wavelengths are presented. Several regions within the same prominence
  are identified for further analysis. Selected profiles for lines
  with formation temperatures between log (T) = 4.7 and log (T) = 6.3,
  as well as their integrated intensities, are given. The profiles of
  coronal, transition region, and He ii lines are discussed. We pay
  special attention to the He ii line, which is blended with coronal
  lines. <BR /> Results: Some quantitative results are obtained by
  analysing the line profiles. They confirm that depression in EUV lines
  can be interpreted in terms of two mechanisms: absorption of coronal
  radiation by the hydrogen and neutral helium resonance continua, and
  emissivity blocking. We present estimates of the He ii line integrated
  intensity in different parts of the prominence according to different
  scenarios for the relative contribution of absorption and emissivity
  blocking to the coronal lines blended with the He ii line. We estimate
  the contribution of the He ii 256.32 Å line to the He ii raster image
  to vary between ~44% and 70% of the raster's total intensity in the
  prominence according to the different models used to take into account
  the blending coronal lines. The inferred integrated intensities of
  the He ii 256 Å line are consistent with the theoretical intensities
  obtained with previous 1D non-LTE radiative transfer calculations,
  yielding a preliminary estimate of the central temperature of 8700 K,
  a central pressure of 0.33 dyn cm<SUP>-2</SUP>, and a column mass of
  2.5 × 10<SUP>-4</SUP> g cm<SUP>-2</SUP>. The corresponding theoretical
  hydrogen column density (10<SUP>20</SUP> cm<SUP>-2</SUP>) is about
  two orders of magnitude higher than those inferred from the opacity
  estimates at 195 Å. The non-LTE calculations indicate that the He
  ii 256.32 Å line is essentially formed in the prominence-to-corona
  transition region by resonant scattering of the incident radiation. <P
  />The movie associated to Fig. 2 is available in electronic form at
  <A href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: 2D radiative-magnetohydrostatic model of a prominence observed
    by Hinode, SoHO/SUMER and Meudon/MSDP
Authors: Berlicki, A.; Gunar, S.; Heinzel, P.; Schmieder, B.;
   Schwartz, P.
2011A&A...530A.143B    Altcode:
  <BR /> Aims: Prominences observed by Hinode show very dynamical and
  intriguing structures. To understand the mechanisms that are responsible
  for these moving structures, it is important to know the physical
  conditions that prevail in fine-structure threads. In the present work
  we analyse a quiescent prominence with fine structures, which exhibits
  dynamic behaviour, which was observed in the hydrogen Hα line with
  Hinode/SOT, Meudon/MSDP and Ondřejov/HSFA2, and simultaneously in
  hydrogen Lyman lines with SoHO/SUMER during a coordinated campaign. We
  derive the fine-structure physical parameters of this prominence and
  also address the questions of the role of the magnetic dips and of
  the interpretation of the flows. <BR /> Methods: We calibrate the
  SoHO/SUMER and Meudon/MSDP data and obtain the line profiles of the
  hydrogen Lyman series (Lβ to L6), the Ciii (977.03 Å) and Svi (933.40
  Å), and Hα along the slit of SoHO/SUMER that crosses the Hinode/SOT
  prominence. We employ a complex 2D radiation-magnetohydrostatic (RMHS)
  modelling technique to properly interpret the observed spectral
  lines and derive the physical parameters of interest. The model
  was constrained not only with integrated intensities of the lines,
  but also with the hydrogen line profiles. <BR /> Results: The slit
  of SoHO/SUMER is crossing different prominence structures: threads
  and dark bubbles. Comparing the observed integrated intensities, the
  depressions of Hα bubbles are clearly identified in the Lyman, Ciii,
  and Svi lines. To fit the observations, we propose a new 2D model
  with the following parameters: T = 8000 K, p<SUB>cen</SUB> = 0.035
  dyn cm<SUP>-2</SUP>, B = 5 Gauss, n<SUB>e</SUB> = 10<SUP>10</SUP>
  cm<SUP>-3</SUP>, 40 threads each 1000 km wide, plasma β is 3.5 ×
  10<SUP>-2</SUP>. <BR /> Conclusions: The analysis of Ciii and Svi
  emission in dark Hα bubbles allows us to conclude that there is no
  excess of a hotter plasma in these bubbles. The new 2D model allows us
  to diagnose the orientation of the magnetic field versus the LOS. The
  40 threads are integrated along the LOS. We demonstrate that integrated
  intensities alone are not sufficient to derive the realistic physical
  parameters of the prominence. The profiles of the Lyman lines and also
  those of the Hα line are necessary to constrain 2D RMHS models. The
  magnetic field in threads is horizontal, perpendicular to the LOS,
  and in the form of shallow dips. With this geometry the dynamics of
  fine structures in prominences could be interpreted by a shrinkage of
  the quasi-horizontal magnetic field lines and apparently is not caused
  by the quasi-vertical bulk flows of the plasma, as Hinode/SOT movies
  seemingly suggest.

---------------------------------------------------------
Title: Synthetic differential emission measure curves of prominence
    fine structures
Authors: Gunár, S.; Heinzel, P.; Anzer, U.
2011A&A...528A..47G    Altcode:
  <BR /> Aims: We use 2D single and multi-thread prominence fine-structure
  models to obtain the synthetic DEM curves. These are then compared
  with the DEM curves derived from observations. <BR /> Methods: We use
  the temperature and electron density structure resulting from the
  2D models and numerically compute the average synthetic DEM curves
  for different orientations of the threads with respect to the line of
  sight. <BR /> Results: We show that the synthetic DEM curves obtained
  by 2D modelling are similar to the DEM curves derived from observations
  of quiescent prominences. <BR /> Conclusions: The DEM curves derived
  from observations, which are most reliable above temperatures of 20
  000 K, can be extended towards cool prominence-core temperatures by
  supplementing them with synthetic DEM values obtained by modelling
  hydrogen Lyman spectra originating mainly at temperatures below 20 000
  K. On the other hand, the observed DEM can constrain the temperature
  structure of the prominence fine structures above the formation
  temperatures of the Lyman spectrum.

---------------------------------------------------------
Title: Solar Research with ALMA
Authors: Karlický, M.; Bárta, M.; Da̧browski, B. P.; Heinzel, P.
2011SoPh..268..165K    Altcode: 2010SoPh..tmp..231K; 2010SoPh..tmp..207K
  The Atacama Large Millimeter/sub-millimeter Array (ALMA) is a large
  interferometer that will consist up to 64 high-precision antennas
  operating in the 31.3 - 950 GHz frequency range. In this frequency
  range, which is largely unexplored, unique observations with a broad
  range of scientific objectives (cosmology, cold universe, galaxies,
  stars and their formation, planets and so on) are expected. Among
  these tasks there is a unique possibility to observe the Sun and to
  address several outstanding issues of solar physics. First, the ALMA
  is briefly described and then the new ESO-ALMA European node (ARC),
  built at Ondřejov Observatory, is presented. In Europe, this ARC is
  the only one oriented to solar physics. Consequently, the requirements
  and limitations for ALMA solar observations, as well as some examples
  of possible solar-oriented ALMA projects, are shown. A procedure of
  the preparation and submission of proposals for ALMA observations
  is mentioned.

---------------------------------------------------------
Title: Solar Flares and the Chromosphere
Authors: Fletcher, L.; Turkmani, R.; Hudson, H. S.; Hawley, S. L.;
   Kowalski, A.; Berlicki, A.; Heinzel, P.
2010arXiv1011.4650F    Altcode:
  A white paper prepared for the Space Studies Board, National Academy
  of Sciences (USA), for its Decadal Survey of Solar and Space Physics
  (Heliophysics), reviewing and encouraging studies of flare physics in
  the chromosphere.

---------------------------------------------------------
Title: Solar Flares and the Chromosphere: A white paper for the
    Decadal Survey
Authors: Hudson, H. S.; Fletcher, L.; Turkmani, R.; Hawley, S. L.;
   Kowalski, A. F.; Berlicki, A.; Heinzel, P.
2010helio2010....1H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Modeling of Solar Flare Plasma and Its Radiation
Authors: Varady, Michal; Kasparova, Jana; Moravec, Zdeněk; Heinzel,
   Petr; Karlicky, Marian
2010ITPS...38.2249V    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Towards a New Formation Flying Solar Coronagraph
Authors: Lamy, P.; Vives, S.; Curdt, W.; Dame, L.; Davila, J.; Defise,
   J. M.; Fineschi, S.; Heinzel, P.; Kuzin, S.; Schmutz, W.; Tsinganos,
   K.; Turck-Chieze, S.; Zhukov, A.
2010ASPC..424...15L    Altcode:
  We briefly describe an investigation aiming at the development of a
  giant solar coronagraph instrument onboard of two satellites, separated
  by about 150 m in formation flight for the detailed observation of the
  solar coronal plasma. The European Space Agency (ESA) has selected this
  instrument as the only payload onboard the Proba 3 satellites which
  will be launched in 2013. The Greek team is developing the command
  control board of the coronagraph.

---------------------------------------------------------
Title: Statistical comparison of the observed and synthetic hydrogen
    Lyman line profiles in solar prominences
Authors: Gunár, S.; Schwartz, P.; Schmieder, B.; Heinzel, P.;
   Anzer, U.
2010A&A...514A..43G    Altcode:
  <BR /> Aims: We analyse a unique set of prominence SOHO/SUMER
  Lyman spectra by comparing it with synthetic spectra obtained by 2D
  multi-thread prominence fine-structure models. <BR /> Methods: We
  employed a novel statistical approach to the analysis of the observed
  and synthetic Lyman spectra. We compared the statistical distributions
  of the line properties of the observed and synthetic Lyman spectra using
  a set of four statistical criteria. <BR /> Results: We demonstrate
  the very good agreement between the observed Lyman spectra and
  synthetic spectra obtained by modelling. <BR /> Conclusions: Our set
  of statistical criteria is well-suited to analyses of the prominence
  Lyman spectra because of its sensitivity to a number of different
  parameters governing the conditions in the prominence fine structures.

---------------------------------------------------------
Title: Physics of Solar Prominences: I—Spectral Diagnostics and
    Non-LTE Modelling
Authors: Labrosse, N.; Heinzel, P.; Vial, J. -C.; Kucera, T.; Parenti,
   S.; Gunár, S.; Schmieder, B.; Kilper, G.
2010SSRv..151..243L    Altcode: 2010SSRv..tmp...34L; 2010arXiv1001.1620L
  This review paper outlines background information and covers recent
  advances made via the analysis of spectra and images of prominence
  plasma and the increased sophistication of non-LTE ( i.e. when there is
  a departure from Local Thermodynamic Equilibrium) radiative transfer
  models. We first describe the spectral inversion techniques that have
  been used to infer the plasma parameters important for the general
  properties of the prominence plasma in both its cool core and the
  hotter prominence-corona transition region. We also review studies
  devoted to the observation of bulk motions of the prominence plasma and
  to the determination of prominence mass. However, a simple inversion
  of spectroscopic data usually fails when the lines become optically
  thick at certain wavelengths. Therefore, complex non-LTE models become
  necessary. We thus present the basics of non-LTE radiative transfer
  theory and the associated multi-level radiative transfer problems. The
  main results of one- and two-dimensional models of the prominences and
  their fine-structures are presented. We then discuss the energy balance
  in various prominence models. Finally, we outline the outstanding
  observational and theoretical questions, and the directions for future
  progress in our understanding of solar prominences.

---------------------------------------------------------
Title: How do unresolved motions affect the prominence hydrogen
    Lyman spectrum.
Authors: Gunar, Stanislav; Schwartz, Pavol; Schmieder, Brigitte;
   Heinzel, Petr; Anzer, Ulrich
2010cosp...38.2830G    Altcode: 2010cosp.meet.2830G
  Space-born observations of quiescent prominences in the hydrogen
  Lyman line series provide a considerable amount of information
  about their structure and physical properties. Lyman line series
  thus represents a focus of several detailed studies. However, the
  substantial asymmetries exhibited by considerable number of observed
  Lyman line profiles present a strong indication for the existence of
  hidden fine-structure dynamics. If attributed merely to the Doppler
  shift effect, these asymmetries would correspond to radial velocities
  of the order of 100 km/s. Such high velocities, however, were never
  observed in quiescent prominences. Typical fine-structure velocities are
  of the order of 10 km/s. To tackle this problem, we have modified our
  2D multi-thread prominence models and randomly assigned line-of-sight
  (LOS) velocities of the order of 10 km/s to each thread. The obtained
  synthetic Lyman spectrum exhibits substantial asymme-tries of the line
  profiles comparable with SOHO/SUMER observations. Moreover, our results
  do indicate that the synthetic Lyman-α profiles may exhibit an opposite
  asymmetry to that of the higher Lyman lines. This is consistent with
  observations which often show opposite asym-metries of these lines at
  the same prominence location. We have demonstrated the agreement of
  synthetic and observed spectra not only by comparing asymmetries of
  individual profiles but also by exploiting statistically significant
  sets of the observed and synthetic data. These results represent an
  important step in our understanding of hidden fine-structure dynamics
  of quiescent prominences.

---------------------------------------------------------
Title: ASPIICS / PROBA-3: a formation flying externally-occulted
    giant coronagraph mission
Authors: Lamy, Philippe; Damé, Luc; Curdt, W.; Davila, J.; Defise,
   J. M.; Fineschi, S.; Heinzel, P.; Howard, R.; Kuzin, S.; Schmutz,
   W.; Tsinganos, K.; Turck-Chièze, S.; Zhukov, A.
2010cosp...38.2858L    Altcode: 2010cosp.meet.2858L
  Classical externally-occulted coronagraphs are presently limited in
  their performances by the distance between the external occulter and
  the front objective. The diffraction fringe from the occulter and
  the vignetted pupil which degrades the spatial resolution prevent
  useful observa-tions of the white light corona inside typically 2-2.5
  Rsun. Formation flying offers an elegant solution to these limitations
  and allows conceiving giant, externally-occulted coronagraphs
  us-ing a two-component space system with the external occulter on
  one spacecraft and the optical instrument on the other spacecraft
  at distances of hundred meters. Such an instrument has just been
  selected by ESA to fly (by the end of 2013) on its PROBA-3 mission,
  presently in phase B, to demonstrate formation flying. It will perform
  both high spatial resolution imaging of the solar corona as well as
  2-dimensional spectroscopy of several emission lines (in partic-ular
  the forbidden line of FeXIV at 530.285 nm) from the coronal base out
  to 3 Rsun using a Fabry-Perot interferometer. The classical design of
  an externally-occulted coronagraph is adapted to the formation flying
  configuration allowing the detection of the very inner corona as close
  as 0.05 Rsun from the solar limb. By tuning the position of the occulter
  spacecraft, it may even be possible to try reaching the chromosphere
  and the upper part of the spicules. ASPIICS/PROBA-3 mission, payload
  and scientific objectives are detailed.

---------------------------------------------------------
Title: 

---------------------------------------------------------
Title: Can purely emissive Ly_beta prominence spectra be
    caused by the line of sight oriented parallelly to the magnetic field?
Authors: Schwartz, Pavol; Gunar, Stanislav; Heinzel, Petr; Schmieder,
   Brigitte
2010cosp...38.2852S    Altcode: 2010cosp.meet.2852S
  Small bright prominence was observed on the SW limb on April 26,
  2007 between 13:01 and 23:50 UT by SUMER spectrograph on-board SoHO
  in hydrogen Lyman line series except the Lyα line. Profiles of the
  Lyβ line are peculiar for a prominence because they do not exhibit any
  central reversals (dips in cores of the lines). This could be explained
  by the fact that the line of sight is parallel with the direction of
  the magnetic field in the prominence. We can investigate this fact
  by a statistical comparison of observed profiles with the synthetic
  ones computed using the 2D multi-thread model of the prominence. We
  use synthetic profiles obtained for various orientations of the
  line of sight with respect to the magnetic field, ranging from
  perpendicular to parallel. Profiles are compared statistically using
  their characteristics such as integral intensities, so-called Lyman
  decrement (ratio of integral intensity of the line to integral intensity
  of the Lyβ line, etc.).

---------------------------------------------------------
Title: Relations between theoretical and observational plasma
    parameters and the radiation of the prominence
Authors: Berlicki, Arkadiusz; Schwartz, Pavol; Schmieder, Brigitte;
   Heinzel, Petr; Gunar, Stanislav
2010cosp...38.2945B    Altcode: 2010cosp.meet.2945B
  On April 26, 2007 the quiescent prominence was observed during the
  coordinated campaign of prominence studies icluding SOT, XRT, and
  EIS on Hinode, MDI, EIT, SUMER, and CDS on SOHO, TRACE, and several
  ground-based observatories. This was the first Hinode-SUMER ob-serving
  campaign. In this analysis we use the data obtained with Hinode/SOT,
  SOHO/SUMER and Multichannel Spectrograph MSDP (Meudon, France). The
  SUMER instrument provide us the UV spectra of the prominence in several
  spectral lines along the 120 arcsec slit crossing the prominence. We
  used the following lines: Lβ, Lγ, Lδ, L , C III and S VI. Using
  these spectra we calculated the integrated intensities along the slit
  for all these lines. We also calculated the integrated intensity of
  the Hα line from the spectroscopic ground-based MSDP observations
  for the same parts of the prominence observed at the same time. These
  intensities were used to calibrate the Hinode/SOT data. Next, we
  analyzed the relations between different observed intensities in these
  lines and compared them with the values obtained from the theoretical
  simulations. We analyzed the correlations between observations and
  theoretical modeling and as a results we estimated the different
  physical parameters of the prominence plasma.

---------------------------------------------------------
Title: Multi-spacecraft observation of a magnetic cloud
Authors: de Lucas, Aline; Dal Lago, Alisson; Schwenn, Rainer; Clúa de
   Gonzalez, Alicia L.; Marsch, Eckart; Lamy, Philippe; Damé, Luc; Curdt,
   W.; Davila, J.; Defise, J. M.; Fineschi, S.; Heinzel, P.; Howard, R.;
   Kuzin, S.; Schmutz, W.; Tsinganos, K.; Turck-Chièze, S.; Zhukov, A.
2010cosp...38.1921D    Altcode: 2010cosp.meet.1921D
  Classical externally-occulted coronagraphs are presently limited in
  their performances by the distance between the external occulter and
  the front objective. The diffraction fringe from the occulter and
  the vignetted pupil which degrades the spatial resolution prevent
  useful observa-tions of the white light corona inside typically 2-2.5
  Rsun. Formation flying offers an elegant solution to these limitations
  and allows conceiving giant, externally-occulted coronagraphs
  us-ing a two-component space system with the external occulter on
  one spacecraft and the optical instrument on the other spacecraft
  at distances of hundred meters. Such an instrument has just been
  selected by ESA to fly (by the end of 2013) on its PROBA-3 mission,
  presently in phase B, to demonstrate formation flying. It will perform
  both high spatial resolution imaging of the solar corona as well as
  2-dimensional spectroscopy of several emission lines (in partic-ular
  the forbidden line of FeXIV at 530.285 nm) from the coronal base out
  to 3 Rsun using a Fabry-Perot interferometer. The classical design of
  an externally-occulted coronagraph is adapted to the formation flying
  configuration allowing the detection of the very inner corona as close
  as 0.05 Rsun from the solar limb. By tuning the position of the occulter
  spacecraft, it may even be possible to try reaching the chromosphere
  and the upper part of the spicules. ASPIICS/PROBA-3 mission, payload
  and scientific objectives are presented.

---------------------------------------------------------
Title: Prominence fine structures and corresponding differential
    emission measures
Authors: Gunar, Stanislav; Heinzel, Petr; Anzer, Ulrich
2010cosp...38.2845G    Altcode: 2010cosp.meet.2845G
  We use the temperature and density structure resulting from multi-thread
  prominence fine-structure models (consisting of individual 2D
  vertical threads) to compute the differential emission measures
  (DEM). We derive the DEM at various positions along the length of
  the foremost thread of the multi-thread model and also for various
  angles between the line-of-sight and the magnetic field. We compare
  the calculated DEM values with those obtained by in-versions from
  the observed intensities of the transition-region UV lines. We show
  that the unresolved fine-structuring of quiescent prominences along a
  particular line-of-sight has consid-erable effect on shape of the DEM
  curve due to fracturing of the prominence-corona transition region into
  many thin layers corresponding to individual prominence fine structures.

---------------------------------------------------------
Title: Photometric analysis of Ellerman bombs .
Authors: Berlicki, A.; Heinzel, P.; Avrett, E. H.
2010MmSAI..81..646B    Altcode:
  Observations of Ellerman bombs (EBs) show them as short-lived,
  compact, and spatially localized emissions that are well observable
  in the wings of the Halpha hydrogen line. The Halpha line profiles
  of EBs are characterized by deep absorption at the line center and
  enhanced emission in the wings with maximum around ± 1 Å from the
  line center, fading beyond ± 5 Å. EBs may also be observed in the
  chromospheric Ca II lines and in the UV as bright points often located
  within active regions. Previous work suggests that EBs may be considered
  as micro-flares and may contribute significantly to the heating of the
  lower chromosphere in newly emerging magnetic flux regions. However,
  it is still not clear at what height in the solar atmosphere the
  emission of EBs originates. In our analysis we used observations of
  EBs obtained in the Halpha line with the Dutch Open Telescope (DOT)
  and in the UV range with the TRACE 1600 Å channel. These one-hour
  long simultaneous sequences obtained with high temporal and spatial
  resolution were used to analyze the relation between the emission in
  the Halpha line and at 1600 Å. The observations show fast variations of
  EB emission in both channels. Comparison between the observed emission
  in Halpha and at 1600 Å and theoretical calculations allowed us to
  draw conclusions about the vertical structure of EBs.

---------------------------------------------------------
Title: Solar quiescent prominences. Filamentary structure and
    energetics
Authors: Heinzel, P.; Anzer, U.; Gunár, S.
2010MmSAI..81..654H    Altcode:
  We present a first attempt to solve the non-LTE radiative-transfer
  problem within a 2D numerical domain consisting of several randomly
  distributed vertical threads. This represents a starting point
  to simulate mutual radiative interaction between such prominence
  threads. The second part of the paper presents our new results which
  concern the radiative equilibrium in prominences and in their fine
  structure. We show that adding the non-hydrogenic radiative losses
  significantly lowers the central equilibrium temperatures. To match the
  observed temperatures, an additional heating seems to be unavoidable.

---------------------------------------------------------
Title: RMHS Modeling of Solar Prominences
Authors: Heinzel, P.
2009AIPC.1171..331H    Altcode:
  In 1976 J. Heasley and D. Mihalas published a seminal paper devoted
  to the modeling of solar prominences. They applied their stellar
  atmospheric code based on the novel complete linearization method to
  model the radiation-magnetohydrostatic (RMHS) coupling in prominences,
  to solve the multilevel transfer problem for a mixture of hydrogen
  and helium and to investigate the prominence energy balance. Their
  results served as a benchmark for future developments in this
  field and today, 33 years after that, we would like to show how
  significantly they influenced the current research. With the link
  to this pioneering work, we will discuss recent progress in the RMHS
  modeling of solar prominences, focused on multidimensional/multithread
  radiative transfer, coupling of non-LTE transfer to MHS, the importance
  of partial redistribution for interpreting strong UV lines etc. New
  light was shed recently on the issues of energy balance, again having
  a direct link to the 1976 paper.

---------------------------------------------------------
Title: Response of optical hydrogen lines to beam heating. I. Electron
    beams
Authors: Kašparová, J.; Varady, M.; Heinzel, P.; Karlický, M.;
   Moravec, Z.
2009A&A...499..923K    Altcode: 2009arXiv0904.2084K
  Context: Observations of hydrogen Balmer lines in solar flares remain an
  important source of information on flare processes in the chromosphere
  during the impulsive phase of flares. The intensity profiles of
  optically thick hydrogen lines are determined by the temperature,
  density, and ionisation structure of the flaring atmosphere, by the
  plasma velocities and by the velocity distribution of particles in
  the line formation regions. <BR />Aims: We investigate the role of
  non-thermal electrons in the formation regions of Hα, Hβ, and Hγ
  lines in order to unfold their influence on the formation of these
  lines. We concentrate on pulse-beam heating varying on a subsecond
  timescale. Furthermore, we theoretically explore possibility that a new
  diagnostic tool exists indicating the presence of non-thermal electrons
  in the flaring chromosphere based on observations of optical hydrogen
  lines. <BR />Methods: To model the evolution of the flaring atmosphere
  and the time-dependent hydrogen excitation and ionisation, we used a
  1-D radiative hydrodynamic code combined with a test-particle code that
  simulates the propagation, scattering, and thermalisation of a power-law
  electron beam in order to obtain the flare heating and the non-thermal
  collisional rates due to the interaction of the beam with the hydrogen
  atoms. To not bias the results by other effects, we calculate only
  short time evolutions of the flaring atmosphere and neglect the plasma
  velocities in the radiative transfer. <BR />Results: All calculated
  models have shown a time-correlated response of the modelled Balmer line
  intensities on a subsecond timescale, with a subsecond timelag behind
  the beam flux. Depending on the beam parameters, both line centres
  and wings can show pronounced intensity variations. The non-thermal
  collisional rates generally result in an increased emission from a
  secondary region formed in the chromosphere. <BR />Conclusions: Despite
  the clear influence of the non-thermal electron beams on the Balmer line
  intensity profiles, we were not able on the basis of our simulations
  to produce any unambiguous diagnostic of non-thermal electrons in the
  line-emitting region, which would be based on comparison of individual
  Balmer line intensity profiles. However, fast line intensity variations,
  well-correlated with the beam flux variations, represent an indirect
  indication of pulsating beams.

---------------------------------------------------------
Title: Examples of Science Cases and Requirements for EST
Authors: Sobotka, M.; Heinzel, P.; Kašparová, J.
2009ASPC..405..455S    Altcode:
  We present various suggestions for the study of flares (fast emission
  variations, heating mechanisms), prominences (fine structure, magnetic
  field, energy balance), and sunspots (umbral structure, heating
  mechanisms, depth and structure of the penumbra, Evershed flow). From
  these cases we derive the requirements for the future European Solar
  Telescope: spectropolarimetric capabilities, high signal-to-noise ratio,
  multi-line spectroscopy, high spatial and temporal resolution.

---------------------------------------------------------
Title: Oscillatory phenomena in a solar network region
Authors: Tsiropoula, Georgia; Tziotziou, Kostas; Schwartz, Pavol;
   Heinzel, Petr
2009IAUS..257..181T    Altcode:
  We examine oscillatory phenomena in a solar network region from
  multi-wavelength, observations obtained by the ground-based Dutch
  Open Telescope (DOT), and by instruments on the spacecraft Solar and
  Heliospheric Observatory (SoHO). The observations were obtained during
  a coordinated observing campaign on October 14, 2005. The temporal
  variations of the intensities and velocities in two distinct regions of
  the quiet Sun were investigated: one containing several dark mottles
  and the other several bright points defining the network boundaries
  (NB). The aim is to find similarities and/or differences in the
  oscillatory phenomena observed in these two regions and in different
  spectral lines formed from the chromosphere to the transition region,
  as well as propagation characteristics of waves.

---------------------------------------------------------
Title: Multiwavelength analysis of a solar quiet region
Authors: Tsiropoula, G.; Tziotziou, K.; Schwartz, P.; Heinzel, P.
2009A&A...493..217T    Altcode:
  Context: We examine oscillatory phenomena in a solar network region
  from multi-wavelength observations obtained by the ground-based Dutch
  Open Telescope (DOT) and by the Coronal Diagnostic Spectrometer (CDS)
  on the spacecraft Solar and Heliospheric Observatory (SoHO). The
  observations were obtained during a coordinated observing campaign in
  October 2005. <BR />Aims: We investigate the temporal variations of the
  intensities and the velocities in two distinct regions of the quiet Sun,
  one containing several dark mottles and the other several bright points
  defining the network boundaries (NB). The aim is to find similarities
  and/or differences in the oscillatory phenomena observed in these two
  regions and in different spectral lines formed from the chromosphere
  to the transition region, as well as the propagation characteristics
  of waves. <BR />Methods: Intensity and velocity variations are
  studied with wavelet and phase difference analyses. <BR />Results:
  Both regions (i.e. mottles and NB) show a periodicity of ~5 min in all
  considered lines. The V-V phase differences in the NB region point to
  an upward propagation of waves; in the region of mottles, for periods
  of 250-400 s, the phase difference is mainly negative, which suggests
  a downward propagation, in turn indicating a refraction of waves from
  the inclined magnetic field of mottles along the line-of-sight. <BR
  />Conclusions: The phase differences at the NB arise from a predominance
  of upward propagating waves. In the mottles' region, the negative phase
  differences we found suggest that propagating waves encounter a boundary
  and are refracted and reflected. Of course, several limitations exist
  in the exact interpretation of the phase differences, e.g. the complex
  topology of the magnetic field, the formation conditions and heights
  of the examined spectral lines, and the low spatial resolution.

---------------------------------------------------------
Title: Far-IR and Radio Thermal Continua in Solar Flares
Authors: Kašparová, J.; Heinzel, P.; Karlický, M.; Moravec, Z.;
   Varady, M.
2009CEAB...33..309K    Altcode: 2009arXiv0901.3465K
  With the invention of new far-infrared (FIR) and radio mm and sub-mm
  instruments (DESIR on SMESE satellite, ESO-ALMA), there is a growing
  interest in observations and analysis of solar flares in this so far
  unexplored wavelength region. Two principal radiation mechanisms play a
  role: the synchrotron emission due to accelerated particle beams moving
  in the magnetic field and the thermal emission due to the energy deposit
  in the lower atmospheric layers. In this contribution we explore the
  time-dependent effects of beams on thermal FIR and radio continua. We
  show how and where these continua are formed in the presence of time
  dependent beam heating and non-thermal excitation/ionisation of the
  chromospheric hydrogen plasma.

---------------------------------------------------------
Title: Electron Densities in Quiescent Prominences Derived from
    Eclipse Observations
Authors: Jejčič, S.; Heinzel, P.
2009SoPh..254...89J    Altcode:
  We develop a diagnostic tool for determination of the electron
  densities in solar prominences using eclipse data. The method is based
  on analysis of the hydrogen Balmer-line intensities (namely Hα and
  Hβ) and the white-light emission due to Thomson scattering on the
  prominence electrons. Our approach represents a generalization of
  the ratio method already used by Koutchmy, Lebecq, and Stellmacher
  (Astron. Astrophys.119, 261, 1983). In this paper we use an extended
  grid of non-LTE prominence models of Gouttebroze, Heinzel, and Vial
  (Astron. Astrophys. Suppl. Ser.99, 513, 1993) and derive various
  useful relations between prominence radiation properties and electron
  densities. Simultaneously, an effective geometrical thickness of the
  prominence can also be obtained. As an example we apply our general
  technique to original eclipse data of Koutchmy, Lebecq, and Stellmacher
  (Astron. Astrophys.119, 261, 1983). Finally, we use our results to
  determine the color of prominences as it should be seen during total
  eclipses.

---------------------------------------------------------
Title: On Lyman-line asymmetries in quiescent prominences
Authors: Gunár, S.; Heinzel, P.; Anzer, U.; Schmieder, B.
2008A&A...490..307G    Altcode:
  Aims: We study the asymmetries of the synthetic hydrogen Lyman
  lines and the process responsible for their formation. <BR
  />Methods: To obtain the synthetic Lyman line profiles, we use a
  multi-thread prominence fine-structure model consisting of identical
  2D threads. The 2D thread models are in MHS equilibrium, include an
  empirical prominence-corona transition region, and solve consistently
  2D non-LTE radiative transfer. Each thread of the multi-thread model
  has a randomly assigned line-of-sight (LOS) velocity. <BR />Results:
  The synthetic Lyman spectrum obtained by multi-thread modelling
  exhibits substantial asymmetries of the line profiles, even though
  the LOS velocities of individual threads are only of the order of 10
  km s<SUP>-1</SUP>. Moreover, our results indicate that the synthetic
  Lyman-α profiles may exhibit an opposite asymmetry to that of the
  higher Lyman lines. <BR />Conclusions: The presence and behaviour
  of the asymmetrical profiles of the synthetic Lyman lines agree with
  observed profiles acquired by SUMER. <P />Appendix A is only available
  in electronic form at http://www.aanda.org

---------------------------------------------------------
Title: NLTE modelling of the flaring atmosphere above sunspot
Authors: Berlicki, A.; Heinzel, P.; Schmieder, B.; Li, H.
2008A&A...490..315B    Altcode:
  Aims: We performed an analysis of the solar flaring atmosphere above
  sunspots. During the flare on October 20, 2003 many flaring structures
  were observed projected onto the sunspots. We analysed the Hα and
  Ca II line profiles emitted by the ribbons partially overlapping the
  sunspots. In the penumbra, the line intensity in the far wings is lower
  than in a typical quiet Sun profile but the core emission of Hα and
  Ca II lines is typical for flares. We tried to find the structure of
  the flare observed above the sunspot penumbra using the observations
  of these chromospheric line profiles. <BR />Methods: NLTE radiative
  transfer techniques allowed us to model the atmosphere of flaring
  structures and fit both the synthetic Hα and Ca II line profiles to
  the observed ones. We have derived semiempirical models of the flaring
  structure observed above sunspots. <BR />Results: Our analysis shows
  that the flare emission observed within the sunspot penumbra comes from
  geometrically thin loop-like structures (cool flare loops) located
  above the fibrils of the penumbra. The structure of the penumbra
  located below the flare is almost not affected by the flare i.e. the
  flare emission in Hα and Ca II comes not from the upper chromosphere
  but from the structures that are higher in the corona. Therefore, a
  two-component modelling is necessary to reproduce the flare emission
  above the sunspot penumbra detected in our observations.

---------------------------------------------------------
Title: Hinode, TRACE, SOHO, and Ground-based Observations of a
    Quiescent Prominence
Authors: Heinzel, P.; Schmieder, B.; Fárník, F.; Schwartz, P.;
   Labrosse, N.; Kotrč, P.; Anzer, U.; Molodij, G.; Berlicki, A.;
   DeLuca, E. E.; Golub, L.; Watanabe, T.; Berger, T.
2008ApJ...686.1383H    Altcode:
  A quiescent prominence was observed by several instruments on
  2007 April 25. The temporal evolution was recorded in Hα by the
  Hinode SOT, in X-rays by the Hinode XRT, and in the 195 Å channel by
  TRACE. Moreover, ground-based observatories (GBOs) provided calibrated
  Hα intensities. Simultaneous extreme-UV (EUV) data were also taken by
  the Hinode EIS and SOHO SUMER and CDS instruments. Here we have selected
  the SOT Hα image taken at 13:19 UT, which nicely shows the prominence
  fine structure. We compare this image with cotemporaneous ones taken
  by the XRT and TRACE and show the intensity variations along several
  cuts parallel to the solar limb. EIS spectra were obtained about half
  an hour later. Dark prominence structure clearly seen in the TRACE and
  EIS 195 Å images is due to the prominence absorption in H I, He I,
  and He II resonance continua plus the coronal emissivity blocking due
  to the prominence void (cavity). The void clearly visible in the XRT
  images is entirely due to X-ray emissivity blocking. We use TRACE, EIS,
  and XRT data to estimate the amount of absorption and blocking. The
  Hα integrated intensities independently provide us with an estimate of
  the Hα opacity, which is related to the opacity of resonance continua
  as follows from the non-LTE radiative-transfer modeling. However,
  spatial averaging of the Hα and EUV data have quite different natures,
  which must be taken into account when evaluating the true opacities. We
  demonstrate this important effect here for the first time. Finally,
  based on this multiwavelength analysis, we discuss the determination
  of the column densities and the ionization degree of hydrogen in
  the prominence.

---------------------------------------------------------
Title: Modelling of the Flare Observed Above Sunspot Penumbra
Authors: Berlicki, A.; Heinzel, P.; Schmieder, B.; Li, H.
2008ESPM...12.3.19B    Altcode:
  The solar flaring atmosphere above sunspot observed during the event
  on October 20, 2003 was analysed. Many flaring structures were visible
  in projection onto the sunspot penumbra. We analysed the H? and Ca
  II line profiles emitted by the ribbons partially overlapping the
  sunspots. These observations were performed with the Multi-channel
  Infrared Solar Spectrograph (MISS) at Purple Mountain Observatory (PMO,
  China). <P />In the sunspot penumbra, the line intensity in far wings
  is lower than in a typical quiet-Sun profile but in the line centre
  the intensity of H? and Ca II lines is typical for flares. Using 1D
  approximation we tried to find the vertical structure of the flare
  observed above sunspot penumbra using the observations of these
  chromospheric line profiles. <P />NLTE radiative transfer techniques
  allowed us to model the atmosphere of flaring structures and fit both
  the synthetic H? and Ca II line profiles to the observed ones. We
  have determined semiempirical models of the flaring structure observed
  above sunspots. <P />In our analysis we showed that the flare emission
  observed within sunspot penumbra comes from geometrically thin loop-like
  structures located above the fibrils of the penumbra. The structure
  of the penumbra located below the flare is almost not affected by
  the flare. The flare emission in chromospheric lines comes not from
  the upper chromosphere but from the structures located higher in the
  corona. Therefore, we performed two-component modelling which well
  reproduce the flare emission above sunspot penumbra. In our model of
  the flaring layer we included the transition region which is necessary
  to obtain agreement between the observed and calculated line profiles.

---------------------------------------------------------
Title: Hydrogen Balmer Lines in the Solar Atmosphere Heated by
    Electron Beams
Authors: Kasparova, J.; Varady, M.; Moravec, Z.; Heinzel, P.;
   Karlicky, M.
2008ESPM...12.3.16K    Altcode:
  Accelerated particle beam are one of the mechanisms of the flare
  energy transport from the corona to the transition region and the
  chromosphere. Such beams heat ambient plasma and may affect atomic
  population via collisions. Using 1D NLTE radiative hydrodynamics
  we model influence of electron beams on hydrogen Balmer lines. In
  the contribution we focus on the effect of so-called non-thermal
  collisional rates on Halpha and Hbeta lines. Based on our results we
  discuss diagnostic methods for determination of beam presence in the
  formation regions of Halpha and Hbeta lines.

---------------------------------------------------------
Title: Understanding the Solar Chromosphere
Authors: Heinzel, P.
2008AIPC.1043..238H    Altcode:
  We discuss the latest high-resolution ground and space-based
  observations of the solar chromosphere and their relevance to problems
  of chromospheric modeling. In particular, we briefly review recent as
  well as previous attempts to understand the solar chromosphere as the
  atmospheric layer with an apparently increasing temperature. Various
  heating mechanisms are also mentioned.

---------------------------------------------------------
Title: Prominence and its Coronal Cavity Observed by Hinode, TRACE
    and SOHO
Authors: Schmieder, B.; Heinzel, P.; Schwartz, P.; Gunar, S.
2008ESPM...12.2.95S    Altcode:
  We will first give a definition of what is a prominence according to
  the glossary of Solar Physicists. A prominence is a filament observed
  at the limb. A filament lies over the inversion line of photospheric
  longitudinal magnetic field and is supported in dips of horizontal
  magnetic field lines. Recent models of flux tubes prove that fine
  structures of prominences could be represented by vertical structures
  embedded in dips of horizontal field lines. <P />Observations of a
  prominence observed in H? by Hinode/SOT and the solar tower of Meudon
  show a very high dynamic nature. SUMER spectra in Lyman series show
  no reverse profiles indicating a large prominence corona transition
  region. <P />This prominence is surrounded by a large coronal cavity
  as show spatial telescopes (TRACE, XRT). <P />These results will be
  discussed in term of different formation models.

---------------------------------------------------------
Title: Far-IR and Radio Continua in Solar Flares
Authors: Heinzel, P.; Kasparova, J.; Varady, M.; Karlicky, M.;
   Moravec, Z.
2008ESPM...12.3.20H    Altcode:
  With the invention of new far-infrared (FIR) and radio mm and sub-mm
  instruments (DESIR on SMESE satellite, ESO ALMA), there is a growing
  interest in observations and analysis of solar flares in this so far
  unexplored wavelength region. Two principal radition mechanisms play a
  role: the synchrotron emission due to accelerated particle beams moving
  in the magnetic field and the thermal emission due to energy deposit
  in the lower atmospheric layers. The latter one was recently explored
  for the case of semiempirical flare models, without considering the
  temporal evolution. However, as the radiation-hydrodynamical simulations
  do show, the lower atmosphere heated by beams exhibits fast temporal
  changes which are typically reflected in variations of spectral-line
  intensities. In this contribution we explore the time-dependent effects
  of beams on FIR and radio continua. We show how and where these
  continua are formed in the presence of time dependent beam heating
  and non-thermal excitation/ionization of the chromospheric hydrogen
  plasma. Our results should contribute to planning of new observations
  in FIR and radio domain.

---------------------------------------------------------
Title: Influence of Seeing on Cloud Model Parameters Obtained from
    Hα Observations
Authors: Tziotziou, K.; Tsiropoula, G.; Heinzel, P.
2008ASPC..397...63T    Altcode:
  We study the influence of atmospheric seeing due to terrestrial
  atmospheric turbulence on cloud model parameters obtained from Hα
  observations with Beckers' cloud model. The analysis indicates that
  atmospheric seeing does not affect the velocity determination, but
  does influence significantly the determination of the Doppler width
  when velocity gradients are present, and hence, the determination of
  the temperature, while the optical thickness and source function are
  also quantitatively affected, especially for high values of atmospheric
  seeing.

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Title: On Lyman-line Asymmetries in Quiescent Prominences
Authors: Gunár, S.; Heinzel, P.; Anzer, U.; Schmieder, B.
2008ESPM...12.3.18G    Altcode:
  We present a new study of the asymmetries of synthetic hydrogen Lyman
  line profiles and suggest the mechanism of their formation. <P />In
  order to obtain the synthetic Lyman line profiles, we use multi-thread
  prominence fine-structure model consisting of identical vertical
  2D threads. The 2D thread models are in magnetohydrostatic (MHS)
  equilibrium, include an empirical prominence-corona transition
  region (PCTR) and consistently solve the 2D non-LTE radiative
  transfer. Individual threads of the multi-thread fine-structure model
  have a randomly assigned LOS velocities. <P />The synthetic Lyman
  spectrum obtained by our multi-thread modelling exhibits substantial
  asymmetries of the line profiles even thought the LOS velocities
  of individual threads are only of the order of 10 km s-1. Moreover,
  our results show that the synthetic Lyman-? profiles may exhibit an
  opposite asymmetry as compared to higher Lyman lines. These results are
  in agreement with the observed Lyman line profiles from SOHO/SUMER. <P
  />The presence and the behaviour of the asymmetrical profiles of the
  synthetic Lyman spectrum is in agreement with observed profiles taken
  by SUMER.

---------------------------------------------------------
Title: Eclipse Observations of Quiescent Prominences
Authors: Jejcic, S.; Heinzel, P.; Kotrc, P.; Druckmuller, M.
2008ESPM...12.2.66J    Altcode:
  In this study we demonstrate how to analyze the solar eclipse data
  taken by a digital camera. We use the observations of a quiescent
  prominence obtained during the total solar eclipse on March 29, 2006
  (Side, Turkey). Using the RGB signal of the white light emission
  and co-temporal H? spectra taken at Ondrejov Observatory, we derive
  the electron density, temperature and geometrical thickness of the
  studied prominence.

---------------------------------------------------------
Title: Solar Prominence Diagnostic with Hinode/EIS
Authors: Labrosse, N.; Schmieder, B.; Heinzel, P.; Gunar, S.
2008ESPM...12.2.21L    Altcode:
  We report here on observations of a solar prominence obtained on 26
  April 2007 using the Extreme Ultraviolet Imaging Spectrometer (EIS)
  on Hinode. Selected profiles for lines with formation temperatures
  between log(T)=4.7 and log(T)=6.3 are given and are used to explain
  the existence of dark features in the raster images. We estimate
  the contribution of the He II 256.32 Å line in the raster image at
  256 Å in the prominence region. We compare the observed prominence
  profiles with theoretical profiles from non-LTE radiative transfer
  models and deduce the contribution of resonant scattering in the He
  II 256 Å emission.

---------------------------------------------------------
Title: Contrast of Fine-scale Structures in a Quiet Sun Network Region
Authors: Schwartz, P.; Tziotziou, K.; Heinzel, P.; Tsiropoula, G.
2008ESPM...12.2.35S    Altcode:
  We study the contrast of fine structures (mottles), found in a quiet-Sun
  network region and close to a filament, observed by the SOHO/SUMER
  spectrograph. The observations were made during August 29 -- 30, 1996,
  in several chromospheric, transition-region and coronal EUV lines. The
  contrasts of the fine-scale structures were obtained in the different
  spectral lines and compared to find whether they have any dependence
  on the inclination of the magnetic field lines and the line formation
  height. Also contributions of the absorption and emissivity blocking
  to the depression of brightness in these fine-scale structures are
  studied by comparing the observations in transition-region lines
  with wavelengths above and below 912 A (the head of the hydrogen
  Lyman continuum).

---------------------------------------------------------
Title: Oscillatory Phenomena in a Solar Network Region
Authors: Tziotziou, K.; Tsiropoula, G.; Schwartz, P.; Heinzel, P.
2008ESPM...12.2.41T    Altcode:
  Multi-wavelength, multi-instrument observations, obtained during a
  coordinated observing campaign on October 2005 by the ground-based
  Dutch Open Telescope (DOT), and by instruments on the spacecraft Solar
  and Heliospheric Observatory (SoHO) and Transition Region and Coronal
  Explorer (TRACE), are used to study oscillatory phenomena in a solar
  network region. Temporal variations of the intensities and velocities
  in a region of the quiet Sun containing several dark mottles and in a
  region with several bright points defining the network boundaries (NB)
  are investigated with the aim of finding similarities and/or differences
  in the oscillatory phenomena observed in these two regions and in
  different spectral lines formed from the chromosphere to the transition
  region, as well as propagation characteristics of waves. A wavelet,
  phase difference and coherence analyses were performed indicating a
  periodicity around 5 min in all considered lines for both regions. V-V
  phase differences in the NB region point to an upward propagation of,
  most probably, acoustic waves, while in the region of mottles they
  indicate a non vertical propagation of waves, due to the presence
  of several inclined mottles along the line-of-sight. In mottles, for
  periods of 250-400 s the phase difference is mainly negative suggesting
  that propagating waves encounter a boundary and are refracted and
  reflected. However, limitations arising from the complex topology
  of the magnetic field, the formation conditions and heights of the
  examined spectral lines and the low spatial resolution of the space
  instruments influence the exact interpretation of the phase differences.

---------------------------------------------------------
Title: Prominence modelling: from observed emission measures to
    temperature profiles
Authors: Anzer, U.; Heinzel, P.
2008A&A...480..537A    Altcode:
  Aims:We outline the construction of prominence - corona transition
  region models based upon the observations of one particular
  prominence. <BR />Methods: The differential emission measure curves from
  observations were approximated by simple analytical functions. On this
  basis we constructed the temperature curve and calculated the radiative
  losses, the gains by thermal conduction, and some estimates for the
  wave heating. <BR />Results: The temperature curve was calculated in
  the range between 23 000 K and 450 000 K. The resulting transition
  region can be divided into an inner region where the temperature is
  low and the radiative losses are very large, a part with a very steep
  temperature rise from 40 000 K to around 250 000 K over a width of only
  500 km, and an extended high temperature region. Both the conductive
  heating and our estimates for a possible wave cooling/heating peak very
  sharply in the region with the very large temperature gradient. The
  consequences for the energy balance are discussed.

---------------------------------------------------------
Title: Modelling of Optical Emission in Solar Flares
Authors: Varady, M.; Kašparová, J.; Heinzel, P.; Karlický, M.;
   Moravec, Z.
2008CEAB...32..101V    Altcode:
  We present recent progress achieved by our group in the field of flare
  optical emission modelling. We concentrate on two problems. Firstly,
  on the possibility of modelling of the time evolution of several Balmer
  line profiles calculated for real electron fluxes obtained from the hard
  X--ray observations of a particular flare with the prospect to compare
  the theoretical results with the observed data for the corresponding
  flare. Secondly, we discuss the influence of the non--thermal electrons
  in the line emitting region on the formation and time evolution of
  Balmer hydrogen line profiles.

---------------------------------------------------------
Title: Multi-wavelength Analysis of a Solar Network Region
Authors: Tsiropoula, G.; Tziotziou, K.; Schwartz, P.; Heinzel, P.
2008CEAB...32..109T    Altcode:
  We analyse co-temporal observations of a network region found near
  the solar disc centre, obtained by the Dutch Open Telescope (DOT)
  and the Coronal Diagnostic Spectrometer (CDS) on-board SOHO during a
  coordinated observing campaign in October 2005. DOT obtained images in
  5 wavelengths along the ha\ profile, while CDS obtained sit-and-stare
  observations in several EUV spectral lines that span the upper solar
  atmosphere. After fitting the CDS spectral line profiles we obtained
  2-D space-time maps of intensities, Doppler velocities and Doppler
  widths. We study the appearance of the network region in the different
  spectral lines and the temporal variations of the obtained physical
  parameters. We employ a wavelet analysis to examine the existence of
  oscillations at the network in the different solar layers.

---------------------------------------------------------
Title: Limb Prominences Seen in UV, EUV and SXR
Authors: Heinzel, P.; Fárník, F.; Anzer, U.; Dammasch, I.
2007ASPC..369..279H    Altcode:
  We use SOHO/SUMER, EIT and Yohkoh/SXT prominence observations to study
  the absorption and/or volume blocking of UV, EUV and SXR coronal
  radiation by cool prominence plasma. An example of such a complex
  behaviour is the limb prominence observed on 5 September 1996. The
  SUMER spectrograph has detected two coronal lines, MgX at 625 Å,
  which is absorbed by the hydrogen Lyman continuum and blocked within
  a volume occupied by cool prominence plasma, and FeXII at 1242 Å,
  where the prominence appears dark due to blocking (no absorption at
  this wavelength). A similar behaviour show also the EUV images taken by
  EIT. We find that a darkening similar to that detected in the FeXII line
  is quite well visible also in the SXR images obtained by Yohkoh/SXT. To
  explain this feature, we exclude the absorption by the HeI and HeII
  resonance continua (hydrogen absorption is quite negligible) and suggest
  that it is entirely due to the volume blocking. Based on a quantitative
  analysis of these data, we discuss the physical conditions in cool
  prominences and their coronal environment. Finally, we propose new
  high-resolution EUV and SXR observations of prominences by Solar-B,
  using the EUV imaging spectrometer (EIS) and the X-ray telescope
  (XRT), respectively.

---------------------------------------------------------
Title: Hydrogen Balmer line formation in solar flares affected by
    return currents
Authors: Štepán, J. Å.; Kašparová, J.; Karlický, M.; Heinzel, P.
2007A&A...472L..55S    Altcode: 2007arXiv0708.0265S
  Aims:We investigate the effect of the electric return currents in
  solar flares on the profiles of hydrogen Balmer lines. We consider the
  monoenergetic approximation for the primary beam and runaway model of
  the neutralizing return current. <BR />Methods: Propagation of the
  10 keV electron beam from a coronal reconnection site is considered
  for the semiempirical chromosphere model F1. We estimate the local
  number density of return current using two approximations for beam
  energy fluxes between 4 × 10<SUP>11</SUP> and 1 × 10<SUP>12</SUP>
  erg cm<SUP>-2</SUP> s<SUP>-1</SUP>. Inelastic collisions of beam and
  return-current electrons with hydrogen are included according to their
  energy distributions, and the hydrogen Balmer line intensities are
  computed using an NLTE radiative transfer approach. <BR />Results:
  In comparison to traditional NLTE models of solar flares that neglect
  the return-current effects, we found a significant increase emission
  in the Balmer line cores due to nonthermal excitation by return
  current. Contrary to the model without return current, the line
  shapes are sensitive to a beam flux. It is the result of variation
  in the return-current energy that is close to the hydrogen excitation
  thresholds and the density of return-current electrons.

---------------------------------------------------------
Title: Influence of seeing effects on cloud model inversions
Authors: Tziotziou, K.; Heinzel, P.; Tsiropoula, G.
2007A&A...472..287T    Altcode:
  Context: Atmospheric seeing due to terrestrial atmospheric turbulence
  is a process that distorts solar ground-based observations. <BR
  />Aims: We study the influence of atmospheric seeing on Hα cloud
  model inversions. <BR />Methods: We use Beckers' cloud model which
  assumes a constant source function to obtain physical parameters from
  observed quiet-Sun Hα profiles, and profiles convolved with a Gaussian
  point spread function that simulates the effect of atmospheric seeing
  on solar observations. <BR />Results: Our analysis indicates that
  atmospheric seeing does not affect the velocity determination, but
  does influence significantly the determination of the Doppler width
  when velocity gradients are present, and hence, the determination of
  the temperature, while the optical thickness and source function are
  also quantitatively affected, especially for high values of atmospheric
  seeing. <BR />Conclusions: The effects of atmospheric seeing on cloud
  model inversions also depend on the actual size of the structures
  under study. For the presented observations, the derived cloud model
  parameter distributions do not change significantly for atmospheric
  seeing up to ∼0.5”.

---------------------------------------------------------
Title: Properties of prominence fine-structure threads derived from
    SOHO/SUMER hydrogen Lyman lines
Authors: Gunár, S.; Heinzel, P.; Schmieder, B.; Schwartz, P.;
   Anzer, U.
2007A&A...472..929G    Altcode:
  Context: The SOHO/SUMER observations provide us for the first time with
  the prominence spectra in the Lyman-α line outside the attenuator
  together with the higher members of the hydrogen Lyman series. <BR
  />Aims: We derive the prominence fine-structure thread properties
  by comparing the SOHO/SUMER hydrogen Lyman series observations with
  the synthetic Lyman lines. <BR />Methods: To obtain the synthetic
  profiles of the Lyman lines, we used 2D prominence fine-structure
  thread models with a PCTR and consistently solved the 2D non-LTE
  multilevel radiative transfer. The trial-and-error method was applied
  to find the model with the best agreement between the synthetic Lyman
  line profiles and the observed ones. <BR />Results: The properties of
  the resulting model with the best match of the synthetic and observed
  line profiles are central (minimum) temperature T<SUB>0</SUB> = 7000
  K, maximum column mass in the centre of the thread M<SUB>0</SUB> =
  1.1×10<SUP>-4</SUP> g cm<SUP>-2</SUP>, horizontal field strength in
  the middle of the thread B<SUB>x</SUB>(0) = 6 Gauss and the boundary
  pressure p<SUB>0</SUB> = 0.015 dyn cm<SUP>-2</SUP>. <BR />Conclusions:
  The Lyman line profiles observed by SOHO/SUMER can be better reproduced
  by using multi-thread models consisting of a set of the 2D prominence
  fine-structure threads placed perpendicularly to the line-of-sight,
  rather than with the single-thread model.

---------------------------------------------------------
Title: Is the magnetic field in quiescent prominences force-free?
Authors: Anzer, U.; Heinzel, P.
2007A&A...467.1285A    Altcode:
  Aims:We describe under which conditions the magnetic fields of quiescent
  prominences are force-free and under which gravity plays the dominant
  role. <BR />Methods: The existing observational determinations of the
  magnetic field are summarised and the calculation of the plasma β
  is outlined. We derive the dependence of β on the prominence weight
  and the field strength. <BR />Results: We show that in many cases of
  well-developed quiescent prominences the field can deviate substantially
  from the force-free situation and gravity fully determines the structure
  of the magnetic dips.

---------------------------------------------------------
Title: Hα with Heating by Particle Beams
Authors: Kašparová, J.; Varady, M.; Karlický, M.; Heinzel, P.;
   Moravec, Z.
2007ASPC..368..441K    Altcode: 2007astro.ph..3800K
  Using 1D NLTE radiative hydrodynamics we model the influence of the
  particle beams on the Hα line profile treating the beam propagation and
  the atmosphere evolution self-consistently. We focus on the influence
  of the non-thermal collisional rates and the return current. Based on
  our results, we propose a diagnostic method for determination of the
  particle beam presence in the formation regions of the Hα line.

---------------------------------------------------------
Title: Prominence Parameters from 2D Modeling of Lyman Lines Measured
    with SUMER
Authors: Gunár, S.; Heinzel, P.; Schmieder, B.; Anzer, U.
2007ASPC..368..317G    Altcode:
  We present SOHO/SUMER observations of a solar prominence in the hydrogen
  Lyman series lines and compare the line profiles with the synthetic
  ones obtained using our 2D prominence modeling. The observations
  contain the Ly-β, Ly-γ, and Ly-δ lines on 25 May 2005. <P />In
  order to derive the prominence parameters we used our 2D fine structure
  models of vertical threads in magnetohydrostatic (MHS) equilibrium. By
  varying the input model parameters (central temperature, boundary
  pressure, magnetic field, central column mass and turbulent velocity)
  we obtained a model having the synthetic Lyman line profiles in good
  agreement with the observed ones. In this way we are able to determine
  the structure of the magnetic dip and the thermodynamical parameters
  in the observed prominence.

---------------------------------------------------------
Title: Multiwavelength Observations of Solar Prominences
Authors: Heinzel, P.
2007ASPC..370...46H    Altcode:
  We briefly review the multiwavelength observations of solar prominences
  and filaments ranging from the infrared up to soft X-rays. We give
  several examples of current observations and mention those specific to
  the total solar eclipses. Our particular focus is on the ultraviolet
  (UV) and extreme-UV images taken in various lines of different species.

---------------------------------------------------------
Title: The Physics of Chromospheric Plasmas
Authors: Heinzel, P.; Dorotovič, I.; Rutten, R. J.
2007ASPC..368.....H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Prominences on the Limb: Diagnostics with UV   EUV Lines and
    the Soft X-Ray Continuum
Authors: Anzer, U.; Heinzel, P.; Fárnik, F.
2007SoPh..242...43A    Altcode:
  In this paper we discuss the two mechanisms by which solar prominences
  on the limb can manifest themselves when observed in coronal UV -
  EUV lines and in the soft X-ray continuum. These mechanisms are the
  absorption in the resonance continua of hydrogen and helium on one hand
  and the reduction of the emissivity in a part of the coronal volume
  occupied by a prominence on the other one. We briefly describe earlier
  observations made with SOHO/SUMER, EIT and Yohkoh/SXT. We then discuss
  how the instruments on the new Japanese satellite Hinode can be used
  for more detailed studies of prominences. We also propose some combined
  observations between the Hinode satellite and the SOHO/SUMER instrument.

---------------------------------------------------------
Title: Non-LTE Analysis of Lyman-Line Observations of a Filament
    with SUMER
Authors: Schwartz, P.; Schmieder, B.; Heinzel, P.
2007ASPC..368..359S    Altcode: 2007arXiv0704.3539S
  We present non-LTE diagnostics of the filament observed by SOHO/SUMER
  on May 27, 2005 in the whole Lyman series. The filament was situated
  close to the disk center. The Lα observations were carried out with
  normal voltage of detector A. The slit was placed at the central part
  of the detector -- outside the Lα attenuator. Therefore, the observed
  profiles of this line could be calibrated reliably.

---------------------------------------------------------
Title: Multi-wavelength Analysis of a Quiet Solar Region
Authors: Tsiropoula, G.; Tziotziou, K.; Giannikakis, J.; Young, P.;
   Schühle, U.; Heinzel, P.
2007ASPC..368..171T    Altcode: 2007arXiv0704.1592T
  We present observations of a solar quiet region obtained by the
  ground-based Dutch Open Telescope (DOT), and by instruments on the
  spacecraft SOHO and TRACE. The observations were obtained during a
  coordinated observing campaign on October 2005. The aim of this work
  is to present the rich diversity of fine-scale structures that are
  found at the network boundaries and their appearance in different
  instruments and different spectral lines that span the photosphere
  to the corona. Detailed studies of these structures are crucial to
  understanding their dynamics in different solar layers, as well as
  the role such structures play in the mass balance and heating of the
  solar atmosphere.

---------------------------------------------------------
Title: Optical and UV Emission of Solar Flares: Multiwavelength
    Observations and Modelling
Authors: Kasparova, J.; Heinzel, P.
2007AGUSMSH22A..07K    Altcode:
  Solar flares reveal themselves in various ranges of electromagnetic
  emission and exhibit temporal variations down to sub-second scale,
  namely during the so-called impulsive phase. This contribution will
  focus on spatial and temporal variations of the optical and UV emissions
  which are thought to be driven by flare energy transport in the form
  of accelerated particles. We will review our current understanding
  of the formation of optical and UV emissions during the impulsive
  phase. Namely, we will discuss recent radiative-hydrodynamic models
  and various physical processes playing an important role in radiation
  transfer and formation of optical and UV spectra. We will also report on
  recent interpretations of observations in various lines and continua and
  discuss their importance for the diagnostics of the flare atmosphere
  structure and the presence of accelerated particles in the emission
  formation regions.

---------------------------------------------------------
Title: White-Light Emission of Solar Prominences
Authors: Jejčič, S.; Heinzel, P.
2007ASPC..368..325J    Altcode:
  Using an extended grid of prominence models we compute the prominence
  white-light (WL) emission due to Thomson scattering and compare it
  with that in Hα. The ratio of the WL emission and the total emission
  can explain the color of prominences as observed during the total
  eclipses and can tell us whether the pink color of prominences is due
  to their intrinsic white-light emission or due to coronal contribution
  at the prominence location. We also show how this ratio depends on
  the prominence electron density, temperature and thickness.

---------------------------------------------------------
Title: The Fine Structure of Solar Prominences
Authors: Heinzel, P.
2007ASPC..368..271H    Altcode: 2007arXiv0705.1464H
  Solar prominences and filaments (prominences projected against the solar
  disk) exhibit a large variety of fine structures which are well observed
  down to the resolution limit of ground-based telescopes. We describe
  the morphological aspects of these fine structures which basically
  depend on the type of a prominence (quiescent or active-region). Then
  we review current theoretical scenarios which are aimed at explaining
  the nature of these structures. In particular we discuss in detail
  the relative roles of magnetic pressure and gas pressure (i.e.,
  the value of the plasma-β), as well as the dynamical aspects of
  the fine structures. Special attention is paid to recent numerical
  simulations which include a complex magnetic topology, energy balance
  (heating and cooling processes), as well as the multidimensional
  radiative transfer. Finally, we also show how new ground-based and
  space observations can reveal various physical aspects of the fine
  structures including their prominence-corona transition regions in
  relation to the orientation of the magnetic field.

---------------------------------------------------------
Title: Hydrogen Hα line polarization in solar flares. Theoretical
    investigation of atomic polarization by proton beams considering
    self-consistent NLTE polarized radiative transfer
Authors: Štěpán, J.; Heinzel, P.; Sahal-Bréchot, S.
2007A&A...465..621S    Altcode: 2007astro.ph..1617S
  Context: We present a theoretical review of the effect of impact
  polarization of a hydrogen Hα line due to an expected proton beam
  bombardment in solar flares. <BR />Aims: Several observations indicate
  the presence of the linear polarization of the hydrogen Hα line
  observed near the solar limb above 5% and preferentially in the radial
  direction. We theoretically review the problem of deceleration of the
  beam originating in the coronal reconnection site due to its interaction
  with the chromospheric plasma, and describe the formalism of the density
  matrix used in our description of the atomic processes and the treatment
  of collisional rates. <BR />Methods: We solve the self-consistent NLTE
  radiation transfer problem for the particular semiempirical chromosphere
  models for both intensity and linear polarization components of the
  radiation field. <BR />Results: In contrast to recent calculations,
  our results show that the energy distribution of the proton beam at Hα
  formation levels and depolarizing collisions by background electrons
  and protons cause a significant reduction of the effect below 0.1%. The
  radiation transfer solution shows that tangential resonance-scattering
  polarization dominates over the impact polarization effect in all
  considered models. <BR />Conclusions: . In the models studied, proton
  beams are unlikely to be a satisfying explanation for the observed
  linear polarization of the Hα line.

---------------------------------------------------------
Title: Spectral Diagnostics of the Magnetic Field Orientation in a
    Prominence Observed with SOHO/SUMER
Authors: Schmieder, B.; Gunár, S.; Heinzel, P.; Anzer, U.
2007SoPh..241...53S    Altcode:
  During several campaigns focused on prominences we have obtained
  coordinated spectral observations from the ground and from space. The
  SOHO/SUMER spectrometer allows us to observe, among others, the
  whole Lyman series of hydrogen, while the Hα line was observed
  by the MSDP spectrograph at the VTT. For the Lyman lines, non-LTE
  radiative-transfer computations have shown the importance of the optical
  thickness of the prominence - corona transition region (PCTR) and its
  relation to the magnetic field orientation for the explanation of the
  observed line profiles. Moreover, Heinzel, Anzer, and Gunár (2005,
  Astron. Astrophys.442, 331) developed a 2D magnetostatic model of
  prominence fine structures that demonstrates how the shapes of Lyman
  lines vary, depending on the orientation of the magnetic field with
  respect to the line of sight. To support this result observationally,
  we focus here on a round-shaped filament observed during three days as
  it was crossing the limb. The Lyman profiles observed on the limb are
  different from day to day. We interpret these differences as being due
  to the change of orientation of the prominence axis (and therefore the
  magnetic field direction) with respect to the line of sight. The Lyman
  lines are more reversed if the line of sight is across the prominence
  axis as compared to the case when it is aligned along its axis.

---------------------------------------------------------
Title: Prominence fine structures in a magnetic
    equilibrium. III. Lyman continuum in 2D configurations
Authors: Gunár, S.; Heinzel, P.; Anzer, U.
2007A&A...463..737G    Altcode:
  Aims:We discuss the behavior of the Lyman continuum profiles
  studied on the grid of 2D vertical-thread models for prominence fine
  structures. <BR />Methods: Multilevel non-LTE transfer calculations for
  a 12-level plus continuum hydrogen model atom are used. <BR />Results:
  Since the Lyman continuum is formed in regions with different
  temperatures for different orientations between the magnetic field
  direction and the line-of-sight, our Lyman continuum modeling, together
  with additional information from Lyman lines, represents a very useful
  tool for the determination of the thread structure. <BR />Conclusions:
  .A comparison between our theoretical Lyman continuum models between
  800 Å and 911 Å with the observed values shows that such a modeling
  can give interesting new constraints on the temperature structure in
  prominence threads.

---------------------------------------------------------
Title: Study of an extended EUV filament using SoHO/SUMER observations
    of the hydrogen Lyman lines
Authors: Schwartz, P.; Heinzel, P.; Schmieder, B.; Anzer, U.
2006A&A...459..651S    Altcode:
  Context: .In previous work we determined the 3D structure of an
  EUV extension of the filament observed by SoHO/CDS on 15 October
  1999. The determination of the 3D structure depends on the optical
  thickness τ<SUB>912</SUB> at the hydrogen Lyman-continuum edge at
  912 Å. The τ<SUB>912</SUB> value was unknown, therefore it was taken
  as a free parameter for the 3D-structure determinations.<BR /> Aims:
  .The plasma properties (including τ<SUB>912</SUB>) of this EUV filament
  are estimated using non-LTE modelling of profiles of the hydrogen Lyman
  lines.<BR /> Methods: .The lines Lβ, Lδ, L ɛ, L6 and L7 were observed
  by SoHO/SUMER with the slit positioned across the EUV filament. In our
  modelling the EUV filament was approximated by a horizontal 1D slab with
  constant pressure and the temperature decreasing vertically from the
  edges to interior of the slab. The values of the geometrical thickness
  of the slab in the EUV extension were taken from its 3D structure
  determined for the τ<SUB>912</SUB> values estimated iteratively. The
  synthetic profiles were fitted to observed ones using the χ<SUP>2</SUP>
  minimization.<BR /> Results: .For the Hα-filament part we obtained
  the expected results: a small geometrical thickness between several
  thousand and 15 000 km, temperatures around 5000 K in the interior and
  around 20 000 K in PCTRs, and pressure ~0.1~dyn~cm<SUP>-2</SUP>. That
  leads to an optical thickness in the Hα line center larger than 1. In
  the EUV extension, temperatures of 10 000-40 000 K in the interior
  and 35 000-50 000 K in the vertically extended PCTRs and a pressure
  of ~0.01~dyn~cm<SUP>-2</SUP> were determined. Such large variations
  of the temperature lead to large variations of τ<SUB>912</SUB>.<BR />
  Conclusions: .The EUV extension is inhomogeneous - areas both optically
  thick and thin at 912 Å are present close to each other. Parts
  optically thick at 912 Å are visible also in Hα as faint and tiny dark
  structures around the very dark and well pronounced Hα filament. The
  volume blocking mechanism is an important mechanism throughout the
  whole EUV extension even in its optically thick parts. The absorption
  dominates only in the Hα-filament part of the EUV filament.

---------------------------------------------------------
Title: Polarization Diagnostics of Proton Beams in Solar Flares
Authors: Stepan, J.; Heinzel, P.; Kasparova, J.; Sahal-Brechot, S.
2006IAUJD...1E..55S    Altcode:
  We review the problem of proton beam bombardment of solar chromosphere
  considering the self-consistent NLTE polarized radiation transfer in
  hydrogen lines. Several observations indicate a linear polarization
  of H-alpha line of the order of 5% or higher and preferentially in
  radial direction. This polarization is often explained as anisotropic
  collisional excitation of the n= 3 level by vertical proton beams. Our
  calculations indicate that deceleration of the proton beam with initial
  power-law energy distribution together with increased electron and
  proton densities in H-alpha forming layers lead to negligible line
  polarization. Thus the proton beams seem not to be a good candidate
  for explanation of the observed polarization degree.

---------------------------------------------------------
Title: Study of a Small-Scale Eruptive Event Observed by SOHO/SUMER
Authors: Tomasz, F.; Régnier, S.; Schwarz, P.; Rybák, J.; Kucera,
   A.; Heinzel, P.; Curdt, W.; Wöhl
2006ESASP.617E..79T    Altcode: 2006soho...17E..79T
  No abstract at ADS

---------------------------------------------------------
Title: What We Have Learned about Prominences and Filaments from
    SOHO/SUMER and CDS Spectral Observations
Authors: Heinzel, P.; Schmieder, B.; Vial, J. -C.
2006ESASP.617E..65H    Altcode: 2006soho...17E..65H
  No abstract at ADS

---------------------------------------------------------
Title: Hα Chromospheric Mottles and their UV/EUV Counterparts Seen
    by SOHO/Sumer
Authors: Tziotziou, K.; Heinzel, P.; Tsiropoula, G.; Schühle, U.
2006ESASP.617E.112T    Altcode: 2006soho...17E.112T
  No abstract at ADS

---------------------------------------------------------
Title: Darkening of Coronal Lines by Limb Prominences Observed
    by SOHO/SUMER
Authors: Dammasch, I. E.; Heinzel, P.; Anzer, U.
2006ESASP.617E..66D    Altcode: 2006soho...17E..66D
  No abstract at ADS

---------------------------------------------------------
Title: Importance of Absorption and Volume Blocking for Line Intensity
    Depression in EUV Filaments
Authors: Schwartz, P.; Schmieder, B.; Heinzel, P.
2006ESASP.617E..75S    Altcode: 2006soho...17E..75S
  No abstract at ADS

---------------------------------------------------------
Title: Prominence Parameters Derived from Hydrogen Lyman-α Spectral
    Profiles Measured by SOHO/SUMER
Authors: Gunár, S.; Teriaca, L.; Heinzel, P.; Schühle, U.
2006ESASP.617E..63G    Altcode: 2006soho...17E..63G
  No abstract at ADS

---------------------------------------------------------
Title: The Dynamics and Structure of the Solar Atmosphere As Obtained
    from Combined SUMER/SOHO and TIP2/VTT Observations
Authors: Tomasz, F.; Régnier, S.; Schwartz, P.; Rybák, J.; Kucera,
   A.; Heinzel, P.; Curdt, W.; Wöhl
2006ESASP.617E..78T    Altcode: 2006soho...17E..78T
  No abstract at ADS

---------------------------------------------------------
Title: New perspectives on prominences as observed by SOHO/SUMER
Authors: Schmieder, B.; Vial, J. -C.; Heinzel, P.
2006sf2a.conf..563S    Altcode:
  We summarize the results of our prominence and filament studies
  based on extensive spectral observations with SOHO/SUMER and CDS
  instruments. During the past decade we have gathered several sets
  of UV and EUV spectral data, containing various emission lines of
  different species. Our main objective was to better understand the
  formation of hydrogen Lyman lines and continuum (using the results
  of complex non-LTE transfer simulations). However we have also
  analysed also UV and EUV lines formed under transition-region and
  coronal conditions. Some highlights of our studies are: reproduction
  of Lyman-line profiles with partial redistribution, understanding the
  role of prominence-corona interface in the formation of Lyman-line
  cores, establishing the effect of the magnetic-field orientation
  on the shape of Lyman lines, discovery of EUV filament extensions
  (invisible in the Hα line) and their explanation, reconstruction of
  a 3D topology of the filament using EUV coronal lines, temperature
  diagnostics based on measurements of the hydrogen Lyman continuum,
  proper explanation of a prominence darkening detected in coronal lines.

---------------------------------------------------------
Title: On the Fine Structure of Solar Filaments
Authors: Heinzel, P.; Anzer, U.
2006ApJ...643L..65H    Altcode:
  High-resolution Hα images of solar filaments show a variety of
  dark fine-structure fibrils, most of them aligned with the magnetic
  field that is sheared with respect to the filament long axis. Here we
  demonstrate how such fibrils can be explained in terms of the magnetic
  field dips produced by realistic mass loading due to plasma condensation
  along the top of a magnetic prominence arcade. Our interpretation is
  supported by (2+1)-dimensional radiation-magnetohydrostatic simulations
  that predict quantitatively the properties of such condensations that
  are suspended in the dipped magnetic field.

---------------------------------------------------------
Title: A periodic arcade model for extended EUV filaments
Authors: Anzer, U.; Heinzel, P.
2006A&A...446..301A    Altcode:
  The extensions of Hα filaments that are observed in EUV spectral lines
  require the presence of cool material in a large volume surrounding
  these filaments. This material can only be supported by magnetic fields
  with dips. Such dips can be generated by a sufficiently strong twisting
  of magnetic flux tubes. In the present paper we have extended earlier
  work to more realistic magnetic field configurations that are periodic
  in the x-direction. We derived approximate equilibria for twisted
  slender flux tubes and determined the region that contains dips. In
  addition we investigated the effects on our models of the mass loading
  due to a heavy prominence. Finally we compared our theoretical models
  with the EUV - observations. We conclude that these types of models
  are capable of explaining the basic features of the observations.

---------------------------------------------------------
Title: Prominence Fine Structures in Amagnetic Equilibrium: a Grid
    Oftwo-Dimensional Models
Authors: Gunár, S.; Heinzel, P.; Anzer, U.
2005ESASP.600E..85G    Altcode: 2005dysu.confE..85G; 2005ESPM...11...85G
  No abstract at ADS

---------------------------------------------------------
Title: Multi-Wavelength Analysis of Plasma Flows during Solar Flares
Authors: Berlicki, A.; Schmieder, B.; Heinzel, P.; Li, H.; Del Zanna,
   G.; Rudawy, P.
2005ESASP.600E..58B    Altcode: 2005dysu.confE..58B; 2005ESPM...11...58B
  No abstract at ADS

---------------------------------------------------------
Title: Physical Parameters of Dark Mottles Derived from High
    Resolution Optical Spectra
Authors: Tsiropoula, G.; Tziotziou, K.; Schwartz, P.; Kotrč, P.;
   Heinzel, P.
2005ESASP.600E..72T    Altcode: 2005ESPM...11...72T; 2005dysu.confE..72T
  No abstract at ADS

---------------------------------------------------------
Title: Non-Lte Modelling of the EUV Filament Based on Soho/sumer
    Observations of the Hydrogen Lyman Lines
Authors: Schwartz, P.; Heinzel, P.; Schmieder, B.
2005ESASP.600E..97S    Altcode: 2005dysu.confE..97S; 2005ESPM...11...97S
  No abstract at ADS

---------------------------------------------------------
Title: Hα Line in Solar Atmosphere Heated by Particle Beams
Authors: Kašparová, J.; Varady, M.; Karlický, M.; Moravec, Z.;
   Heinzel, P.
2005ESASP.600E.127K    Altcode: 2005dysu.confE.127K; 2005ESPM...11..127K
  No abstract at ADS

---------------------------------------------------------
Title: Prominence fine structures in a magnetic equilibrium. II. A
    grid of two-dimensional models
Authors: Heinzel, P.; Anzer, U.; Gunár, S.
2005A&A...442..331H    Altcode:
  We construct a grid of 2D vertical-thread models for prominence fine
  structures which are in magnetohydrostatic (MHS) equilibrium. Such
  thread models have been described in a previous paper by Heinzel
  &amp; Anzer (2001), but here we use a modified 2D transfer code with
  an adaptive MHS grid. Multilevel non-LTE transfer calculations are
  now performed for a 12-level plus continuum hydrogen model atom,
  in order to study the behaviour of the Lyman-series lines observed
  by SOHO/SUMER. Our grid consists of 18 models which cover a range of
  central column masses, magnetic-field intensities and two parameters
  characterising the 2D temperature structure of the thread. Since
  different Lyman lines and their parts (line center, peak, wings) are
  formed at different places within the thread, the Lyman series may
  serve as a good diagnostic tool for thermodynamic conditions varying
  from central cool parts to a prominence-corona transition region. We
  demonstrate this behaviour for various lines, showing their synthetic
  profiles as seen from two perpendicular directions along and across
  the magnetic field lines, respectively, and displaying the respective
  contribution functions. This study confirms our earlier conclusion
  that the Lyman line profiles are much more reversed when seen across
  the field lines, compared to those seen along the lines. The latter
  can be even unreversed. We also show the geometrical cross-section
  (shape) of all 18 models. Their thread-like shape with a considerable
  aspect ratio resembles recent high-resolution Hα images. Finally,
  we discuss the relation of our thread models to the vertical threads
  studied by Fontenla et al. (1996, ApJ, 466, 496).

---------------------------------------------------------
Title: On the Nature of Dark Extreme Ultraviolet Structures Seen by
    SOHO/EIT and TRACE
Authors: Anzer, U.; Heinzel, P.
2005ApJ...622..714A    Altcode:
  Spectral lines in the extreme ultraviolet (EUV) observed on the Sun
  can originate either from the hot corona or the cooler chromosphere
  to corona transition region. In the present paper we concentrate on
  coronal lines and in particular on iron lines at 171, 195, and 284
  Å, which have been frequently observed by the Solar and Heliospheric
  Observatory (SOHO)/Extreme Ultraviolet Imaging Telescope (EIT) and the
  Transition Region and Coronal Explorer (TRACE). The intensity of these
  lines emitted by the corona can be reduced by the presence of a cool
  gas, e.g., by prominence-like material, located in the corona. There
  are two mechanisms that can lead to a reduction of the line intensity:
  absorption and volume blocking. That part of the coronal radiation
  that comes from behind the cool gas can be partially absorbed. The
  main absorbers for the iron lines studied here are neutral hydrogen
  and neutral plus singly ionized helium. In this paper we calculate
  the optical thickness of their resonance continua at the wavelength
  positions of iron lines and compare it with that in the Hα line
  center. The comparison of the derived values shows that they are quite
  similar. The second effect is due to the fact that cool structures in
  the corona do not emit any radiation in the EUV lines, which gives rise
  to an additional reduction of the observed intensity as compared with
  the surrounding corona-we have termed this “volume blocking.” We
  further describe in this paper how these two effects can be used in
  a new way of performing prominence diagnostics. Our results are also
  applicable to other coronal lines detected by, e.g., the SOHO CDS or
  SUMER instruments.

---------------------------------------------------------
Title: Non-LTE diagnostics of velocity fields during the gradual
    phase of a solar flare
Authors: Berlicki, A.; Heinzel, P.; Schmieder, B.; Mein, P.; Mein, N.
2005A&A...430..679B    Altcode:
  We perform an analysis of the velocity field within the Hα ribbons
  during the gradual phase of an M 1.0 solar flare observed on October 22,
  2002. We use spectroscopic observations performed with the German VTT
  (Vacuum Tower Telescope) working in the MSDP (Multichannel Subtractive
  Double Pass spectrograph) observing mode. From these observations
  the Hα line profiles in chosen areas of the flare ribbons were
  reconstructed and these observational profiles were compared with
  a grid of synthetic Hα line profiles calculated by the non-LTE
  radiative-transfer code. This code allows us to calculate different
  models of the chromosphere with a prescribed velocity field. By
  optimising the best fit between the observed and synthetic profiles
  we find the most appropriate models of the chromosphere and vertical
  structure of the velocity field in the analysed areas of the flare
  ribbons. By means of the non-LTE radiative-transfer calculations
  we show that in most analysed areas of the Hα flare ribbons the
  chromospheric plasma exhibited upward motion with a mean velocity of
  a few km;s<SUP>-1</SUP>. These results are consistent with previous
  estimates and support the scenario of a gentle evaporation during the
  gradual phase.

---------------------------------------------------------
Title: Physics of Solar Prominences
Authors: Heinzel, P.; Anzed, U.
2005ASSL..320..115H    Altcode: 2005smp..conf..115H
  No abstract at ADS

---------------------------------------------------------
Title: Diagnostics of Dark Chromospheric Mottles Based on High
    Resolution Spectra I - Observational Data
Authors: Kotrč, P.; Schwartz, P.; Heinzel, P.; Tsiropoula, G.;
   Tziotziou, K.
2005HvaOB..29..289K    Altcode:
  High resolution optical spectra of dark mottles in H and Ca lines
  were observed with the Echelle spectrograph of the VTT at Sacramento
  Peak Observatory. Until now, only Hα spectra and slit-jaw images
  were processed. Used methods of identification of the dark mottles in
  the slit-jaw images and in the spectra, as well as a calibration and
  correction on the scattered light are described. Individual steps of
  the procedure, as well as crucial problems are discussed. The finally
  processed line profiles <P />are comparable to the profiles of dark
  mottles obtained by other instruments including MSDP.

---------------------------------------------------------
Title: Influence of Electron Beam Pulses on Hα Line Formation
Authors: Varady, M.; Kašparova, J.; Karlický, M.; Heinzel, P.;
   Moravec, Z.
2005HvaOB..29..167V    Altcode:
  In this contribution we present results of our simulations focused on
  determination of spectroscopic signs of the presence of non--thermal
  electrons in the formation region of Hα using three mutually
  communicating codes. The originally autonomous and highly specialised
  codes model three simultaneously acting processes in flares: the
  precipitation and energy dissipation of the non-thermal power--law
  electron beams in the solar atmosphere, the hydrodynamic response of
  the atmosphere to the energy deposited by the beams, and the radiative
  transfer in chromosphere and photosphere which determines the hydrogen
  line profiles and their time evolution. The results show possible
  existence of a new diagnostic method on presence of electron beams in
  the formation region of the Hα line.

---------------------------------------------------------
Title: Determination of the 3D structure of an EUV-filament observed
    by SoHO/CDS, SoHO/SUMER and VTT/MSDP
Authors: Schwartz, P.; Heinzel, P.; Anzer, U.; Schmieder, B.
2004A&A...421..323S    Altcode:
  Heinzel et al. (\cite{hein1}) found that filaments seem to be much
  more extended in EUV spectral lines than in Hα. In this paper we
  reconstruct the 3D structure of the extensions of the EUV-filament
  observed on 15 October 1999 by SoHO/CDS and SoHO/SUMER. Small Hα
  structures were observed by VTT/MSDP. We computed the bottom and top
  heights of the EUV-filament extensions for several values of the
  hydrogen Lyman-continuum optical thickness τ<SUB>912</SUB> using
  the spectroscopic model of Heinzel et al. (\cite{hein2}). For this
  we used CDS observations of the two coronal lines Mg X 624.94 Å and
  Si XII 520.60 Å. Further, we develop a new method for estimating
  τ<SUB>912</SUB> using the O V line measured by CDS and the O VI
  measured by SUMER onboard SoHO. The latter line is used as a proxy to
  deduce the intensity variations of O V underneath the filament. This
  method also takes into account the presence of prominence-corona
  transition regions. <P />Resulting heights of the EUV-filament
  extensions are around 15 000 km for the bottom and around 40 000 km
  for the top boundaries. However, there are significant variations
  around these representative values and we show that in about half
  of observed pixels the Lyman-continuum absorption dominates in
  the coronal-line depression, while in the other half it is the
  volume blocking effect. The latter situation corresponds to a large
  (larger than 30 000 km) geometrical thickness of the EUV-filament
  extension. From the heights of the boundaries of the EUV-filament the
  geometrical thickness can be computed and used to estimate the total
  mass loading which was found to be comparable to that of typical CMEs.

---------------------------------------------------------
Title: Soft X-ray heating of the solar chromosphere during the
    gradual phase of two solar flares
Authors: Berlicki, A.; Heinzel, P.
2004A&A...420..319B    Altcode:
  In this paper we perform an analysis of the energetics of the solar
  flaring chromosphere irradiated by soft X-rays (SXR) emitted from
  overlying hot flare loops. To study an expected SXR heating we used
  the observations of two solar flares obtained with the Multichannel
  Subtractive Double Pass (MSDP) spectrograph attached to the Large
  Coronagraph of the Wrocław University. SXR observations of these flares
  come from the Yohkoh SXR telescope (SXT). From MSDP spectral images
  we derived mean Hα line profiles which were then used to construct
  semi-empirical non-LTE models of the chromosphere in the analyzed areas
  of flares. On the basis of SXR observations we calculated the mean
  emission measure EM and the temperature in flaring coronal structures
  located above the Hα kernels under study and these two quantities were
  used to compute the SXR irradiation of the chromosphere between 1-300
  Å. For each flare model we then evaluated the energy deposit due to
  such irradiation and compared it with the net radiative cooling rates
  at all depths in the chromosphere. By means of such modelling we were
  able to demonstrate that the enhanced emission of selected Hα kernels
  observed during the gradual phase of these two solar flares cannot be
  explained in terms of the SXR heating of the chromosphere. We found
  that radiative losses in all layers of the chromosphere exceeded
  the amount of the energy deposited by the SXR radiation. However,
  for stronger flares with much enhanced EM a certain contribution of
  SXR to the heating cannot be ruled out.

---------------------------------------------------------
Title: Multi-wavelength study of a high-latitude EUV filament
Authors: Schmieder, Brigitte; Lin, Yong; Heinzel, Petr; Schwartz, Pavol
2004SoPh..221..297S    Altcode:
  A large filament was observed during a multi-wavelength coordinated
  campaign on June 19, 1998 in the Hα line with the Swedish Vacuum Solar
  Telescope (SVST) at La Palma, in the coronal lines Fe ix/x 171 Å and
  Fe xi 195 Å with the Transition Region and Coronal Explorer (TRACE)
  and in EUV lines with the SOHO/CDS spectrometer and the hydrogen Lyman
  series with the SOHO/SUMER spectrometer. Because of its high-latitude
  location, it is possible to disentangle the physical properties of the
  Hα filament and the filament channel seen in EUV lines. TRACE images
  point out a dark region fitting the Hα fine-structure threads and a
  dark corridor (filament channel), well extended south of the magnetic
  inversion line. A similar pattern is observed in the CDS EUV-line
  images. The opacity of the hydrogen and helium resonance continua at
  171 Å is almost two orders of magnitude lower than that at the Hi head
  (912 Å) and thus similar to the opacity of the Hα line. Since we do
  not see the filament channel in Hα, this would imply that it should
  also be invisible in TRACE lines. Thus, the diffuse dark corridor is
  interpreted as due to the coronal `volume blocking' by a cool plasma
  which extends to large altitudes. Such extensions were also confirmed by
  computing the heights from the projection geometry and by simulations
  of the CDS and TRACE line intensities using the spectroscopic model
  of EUV filaments (Heinzel, Anzer, and Schmieder, 2003). Finally,
  our NLTE analysis of selected hydrogen Lyman lines observed by SUMER
  also leads to a conclusion that the dark filament channel is due to
  a presence of relatively cool plasma having low densities and being
  distributed at altitudes reaching the Hα filament.

---------------------------------------------------------
Title: Collisional excitation and ionization of hydrogen by return
    current in solar flares
Authors: Karlický, M.; Kašparová, J.; Heinzel, P.
2004A&A...416L..13K    Altcode:
  First a problem of the transport of electron beams with high energy
  fluxes into the cold chromosphere during the flare is presented. Then
  it is shown that the problem might be solved by the return current
  formed by superthermal (runaway) electrons. In such a case the
  return current electrons could influence hydrogen excitations and
  ionizations. Therefore, we computed collisional rates of such a
  return current and compared them with those of the thermal plasma
  and of a monoenergetic (10 keV) electron beam with the energy flux
  F<SUB>E</SUB> = 10<SUP>12</SUP> erg cm<SUP>-2</SUP> s<SUP>-1</SUP>
  penetrating into the flare atmosphere described by the F1 model (Machado
  et al. \cite{Machado1980}). We show that in this situation the return
  current collisional rates can be dominant for some transitions.

---------------------------------------------------------
Title: Collisional Excitation and Ionization of Hydrogen by Return
    Current in Solar Flares
Authors: Kašparová, J.; Heinzel, P.; Karlický, M.
2004IAUS..219..760K    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Parameters of dark mottles based on high resolution optical
    spectra
Authors: Kotrc, P.; Heinzel, P.; Tziotziou, K.; Tsiropoula, G.
2004IAUS..223..275K    Altcode: 2005IAUS..223..275K
  High resolution optical spectra of hydrogen and calcium lines
  observed with the Echelle spectrograph of the VTT at Sacramento Peak
  Observatory were analyzed. The observed line profiles in some parts
  of dark chromospheric mottles are to be matched with theoretical ones
  using the cloud model and several parameters (e.g. the temperature,
  gas pressure, flow velocity) are to be derived. Individual steps of
  the procedure, as well as crucial problems are discussed.

---------------------------------------------------------
Title: Multi-Wavelength Observations of an M1.0 Flare on 22 October
    2002
Authors: Berlicki, A.; Schmieder, B.; Vilmer, N.; Mein, P.; Mein,
   N.; Heinzel, P.; Staiger, J.; Deluca, E. E.
2004IAUS..219..669B    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Multiwavelength determination of the density and total mass
    of the EUV filament observed by SoHO/CDS, SoHO/SUMER and MSDP/VTT
Authors: Schwartz, P.; Schmieder, B.; Heinzel, P.; Anzer, U.
2004IAUS..223..219S    Altcode: 2005IAUS..223..219S
  It was found that filaments observed in EUV could be much more extended
  than in Halpha. These extended dark structures visible in EUV are named
  EUV filaments. Their parts seen only in EUV (not observable in Halpha
  because of low opacity at the Halpha wavelength) are called EUV-filament
  extensions (or simply EUV extensions). For the EUV filament observed
  by SoHO on 15 October 1999 as northern polar crown filament, only
  a few small dark structures were seen in Halpha. This suggests that
  the mass of the EUV extension is larger than, or at least comparable
  with, the mass of the parts of the filament observed in Halpha. In
  our previous work we determined the 3D structure of the EUV extension
  of this EUV filament. In this paper we present the determinations of
  mass and average density of this EUV extension. For better density
  estimates we interpret the hydrogen Lyman lines observed by SUMER
  using non-LTE radiative transfer code. From the best fitting of Lyman
  lines we obtained a reasonable model of the EUV extension with low gas
  pressure, temperatures from 2times10^4 K to 10^5 K and with extended
  prominence-corona transition regions.

---------------------------------------------------------
Title: A Spectroscopic Model of euv Filaments
Authors: Heinzel, P.; Anzer, U.; Schmieder, B.
2003SoPh..216..159H    Altcode:
  We propose a new spectroscopic model for extended dark structures
  around Hα filaments observed in EUV lines. As in previous papers,
  we call these structures EUV filaments. Our model uses at least three
  observed EUV lines (located shortward the hydrogen Lyman-continuum
  limit) to compute iteratively the altitudes at which the EUV filament
  extensions are located. A transition-region line (O v in the present
  case) can be used to derive the opacity of the Lyman continuum and the
  other two coronal lines (e.g., Mg x and Si xii) then give two heights:
  the bottom and top of the EUV filament. The method takes into account
  self-consistently the absorption of EUV-line radiation by the Lyman
  continuum, as well as the volume-blocking effect potentially important
  for coronal lines. As an example we compute the heights of the EUV
  filament at one particular position, using CDS data for the 5 May 2000
  filament. At this position, the EUV filament extension lies between
  altitudes 28 700 and 39 000 km, so that the geometrical thickness of the
  structure is 10300 km (we discuss also the sensitivity of our models
  to variations of the line intensities). These heights are consistent
  with the concept of twisted magnetic flux tubes, but there could be
  also some influence on our results due to additional low lying cool
  structures from parasitic polarities.

---------------------------------------------------------
Title: Determination of the 3D-topology of an EUV-filament observed
    by SoHO/CDS SoHO/SUMER and VTT/MSDP
Authors: Schwartz, P.; Heinzel, P.; Schmieder, B.; Anzer, U.
2003ESASP.535..495S    Altcode: 2003iscs.symp..495S
  We have constructed a spatial model of an extended EUV-filament
  observed on 15 October 1999 (polar crown N 38 deg) by SoHO/CDS. The
  narrow Hα counterparts were observed by VTT/MSDP. As found in 2001,
  EUV-filaments are much more extended than those parts visible in Hα. We
  have computed the bottom and top heights of this EUV-filament for the
  whole CDS raster for different values of the Lyman-continuum optical
  thickness using CDS measurements of two coronal lines (Mg X 624.94
  Å and Si XII 520.60 Å) and the model of Heinzel et al., 2003. For
  the scale height of the MgX line we used the value from Fludra et
  al. 1999, assuming that this line is not solar cycle and activity
  dependent. We created a new method for τ<SUB>912</SUB> determination
  from O VI and O V line intensities. Because of the inhomogeneity in
  the O V 629.37 Å line intensity distribution in the vicinitiy of
  the EUV-filament it was not possible to estimate this intensity under
  the filament. So we used observations made by SoHO/SUMER of the O VI
  1031.91 Å line not absorbed by EUV-filament cold plasma. The knowledge
  of the heights of the bottom and top boundaries of an EUV-filament
  gives us the EUV-filament geometrical thickness. From this the mass
  of the EUV-filament was computed.

---------------------------------------------------------
Title: EUV-filaments and their mass loading
Authors: Heinzel, P.; Anzer, U.; Schmieder, B.; Schwartz, P.
2003ESASP.535..447H    Altcode: 2003iscs.symp..447H
  It was found recently (Heinzel et al., 2001; Schmieder et al., 2003)
  that solar filaments observed in EUV lines by SOHO/CDS are much more
  extended than their Hα counterparts. This was explained by a large
  difference between the hydrogen Lyman-continuum and Hα opacities. Two
  different MHD models were suggested to explain the EUV-filament
  extensions: the model based on parasitic polarities (Aulanier &amp;
  Schmieder, 2002) and the model with twisted flux tubes (Anzer &amp;
  Heinzel, 2003). The latter model can explain our recent findings
  that at least some parts of the EUV-filament extensions are located
  relatively high in the corona. These heights can be computed using a
  new spectroscopic model of EUV-filaments. The mass which is loaded into
  the EUV-filament extensions is then estimated on the basis of non-LTE
  transfer calculation. The total filament mass is larger than that
  derived for the Hα filament itself and this may have consequences
  for the structure and mass loading of CMEs whenever they form from
  such filaments - this may answer the question how the extended CME
  structures can form from rather narrow Hα filaments. We summarize
  the basic properties of EUV-filaments, present their spectroscopic
  analysis and give some estimates for mass loading. We then discuss
  possible relations between EUV-filaments and CMEs, in particular the
  problems of their masses.

---------------------------------------------------------
Title: On the nature of extended EUV filaments
Authors: Anzer, U.; Heinzel, P.
2003A&A...404.1139A    Altcode:
  This paper describes the properties of extended EUV filaments and the
  theoretical modelling of them. We summarise the general aspects of the
  depression of EUV-line emission and give an interpretation of recent
  filament observations in transition-region and coronal lines. The
  EUV filament was found to be located relatively high in the corona
  (at least 20 000 km above the solar surface) and this requires an
  MHD scenario alternative to the parasitic-polarity model of Aulanier
  &amp; Schmieder (\cite{Aulanier02}). Here we present a new idea
  for the support of cool gas in the magnetic arcade of a prominence
  which is capable of explaining both wide and vertically extended EUV
  filaments. Our mechanism is based upon the twisting of individual
  flux tubes, similar to the one which was suggested by Priest et
  al. (\cite{Priest89}). Finally, the consequences of this new model
  are discussed.

---------------------------------------------------------
Title: Spectroscopic diagnostics of an Hα  and EUV filament observed
    with THEMIS and SOHO
Authors: Schmieder, B.; Tziotziou, K.; Heinzel, P.
2003A&A...401..361S    Altcode:
  A long filament has been observed with THEMIS/MSDP and SOHO/CDS -
  SUMER, during a coordinated campaign (JOPs 131/95) on May 5, 2000. The
  data were (a) 2-D Hα spectra, observed using THEMIS, (b) Lyman series
  spectra and Lyman continuum, observed using SOHO/SUMER, and (c) EUV
  spectra (in O V 629 Å, Mg X 624 Å, Si Xii 520 Å, Ca X 557 Å and
  He I 584 Å) observed using SOHO/CDS. A large depression of the line
  emissions in CDS images represents the EUV filament. A computed model
  shows that the EUV filament consists of an extended in height cloud of
  low gas pressure at an altitude lower than the top of the Hα filament,
  volume-blocking and absorbing coronal emission and absorbing transition
  region line emission. The optical thickness of the Lyman continuum is
  estimated by using the ratio of O V intensity inside and outside the
  EUV filament, while the optical thickness of Hα is computed from the
  Hα line profile by using an inversion technique. Using simultaneous
  Hα , Lyman lines and Lyman continuum spectroscopic data, we performed
  detailed, non-LTE radiative transfer diagnostics of the filament plasma
  conditions. The optical thickness of the Lyman continuum is larger than
  that of the Hα line by one to two orders of magnitude. This could be
  of a great importance for filament formation modeling, if we consider
  that more cool material exists in filament channels but is optically
  too thin to be visible in Hα images.

---------------------------------------------------------
Title: 2D Radiative Transfer in Magnetically Confined Structures
Authors: Heinzel, P.; Anzer, U.
2003ASPC..288..441H    Altcode: 2003sam..conf..441H
  Magnetically confined structures in the solar atmosphere exhibit
  a large complexity in their shapes and physical conditions. As an
  example, we show the case of so-called magnetic dips in prominences
  which are in magnetohydrostatic equilibria. For such models we solve
  2D non-LTE multilevel problem for hydrogen with PRD in Lyman resonance
  lines. The iterative technique used is based on the MALI approach with
  simple diagonal ALO and SC formal solver. <P />To compute the hydrogen
  ionization balance, the preconditioned MALI equations are linearized
  with respect to atomic level populations and electron density and
  solved iteratively using the Newton-Raphson scheme. Two additional
  problems are addressed: (i) an adequate iteration method for cases when
  the column-mass scale is used in one of the two dimensions but varies
  along the other dimension (which has a geometrical scaling); and (ii)
  a possibility of using AMR (Adaptive Mesh Refinement) algorithms to
  account for steep 2D gradients of selected variables (temperature,
  density, etc.).

---------------------------------------------------------
Title: Transport of Energy from the Corona to the Chromosphere
    During Flares
Authors: Heinzel, P.; Karlický, M.
2003LNP...612..161H    Altcode: 2003ecpa.conf..161H
  Hard X-ray (HXR) observations frequently exhibit fast temporal
  variations during the impulsive phase of solar flares and this
  is usually ascribed to the propagation of beams of accelerated
  particles and to the dissipation of their energy in lower layers of
  the solar atmosphere. As a result of fast heating and non-thermal
  processes, several chromospheric lines show significant impulsive
  brightenings. We first review observational attempts of detecting
  such fast (sub-second) variations of the line intensities, namely
  in the Halpha line, and discuss the problems associated with such
  observations. Second, we describe new radiation-hydrodynamical (RHD)
  simulations of the pulse-beam heating and show how they predict both
  HXR and optical-line intensity variations on very short time scales. We
  also discuss the effect of the return current on the energy deposit in
  the atmosphere. Using new spatially-resolved HXR observations (RHESSI)
  made simultaneously with a high-cadence detection of selected optical
  lines, one should be able to diagnose the properties of particle beams,
  provided that the response of the lower atmospheric layers to beam
  pulses is strong enough.

---------------------------------------------------------
Title: Understanding solar flares from optical observations: How do
    particle beams affect the lower atmosphere?
Authors: Heinzel, P.
2003AdSpR..32.2393H    Altcode:
  During the impulsive phase of solar flares, both hard X-ray (HXR) and
  optical emissions exhibit fast temporal fluctuations detectable down
  to sub-second scales. This is usually ascribed to the propagation
  of beams of accelerated particles and to the dissipation of their
  energy in lower layers of the solar atmosphere. Although it is rather
  difficult to prove a temporal correlation between HXR and optical
  intensity variations, we discuss here some previous results and
  recent attempts. Namely in coordination with RHESSI observations,
  several ground-based observatories started to detect fast optical
  variations in the H α line. In addition to this, we also mention a
  possibility of using some other diagnostically important lines. The
  proper interpretation of coordinated HXR and optical observations
  further requires robust tools for radiation-hydrodynamical (RHD) forward
  modeling. We briefly describe a new 'hybrid' code which consists of RHD
  part and particle-simulation part. Short-duration heating due to beam
  pulses is modeled which allows us to predict temporal fluctuations of
  HXR and selected optical and UV lines formed in chromospheric layers and
  in the transition region. Particularly the line asymmetries originating
  in a highly dynamical lower atmosphere of the flare can be used to
  diagnose the response of these layers to particle beams.

---------------------------------------------------------
Title: Soft X-ray Heating of Stellar Chromospheres
Authors: Heinzel, P.; Berlicki, A.
2003IAUS..210P.B15H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Time-dependent Flare Models with MALI
Authors: Kašparová, J.; Heinzel, P.; Varady, M.; Karlický, M.
2003ASPC..288..544K    Altcode: 2003sam..conf..544K
  Temporal variations of Hα line profile intensities related to electron
  beams are presented. We show first results of time dependent simulations
  of a chromospheric response to a 1 sec monoenergetic electron beam. 1-D
  hydrodynamic code together with particle representation of the beam have
  been used to calculate atmospheric evolution. Time dependent radiative
  transfer problem has been solved for the resulting atmosphere in the
  MALI approach, using the Crank-Nicholson implicit scheme. Non-thermal
  collisional rates were included in linearised equations of statistical
  equilibrium.

---------------------------------------------------------
Title: Time dependent flare model with non-LTE radiative transfer
Authors: Varady, M.; Karlický, M.; Kašparová, J.; Heinzel, P.
2002ESASP.506..521V    Altcode: 2002svco.conf..521V; 2002ESPM...10..521V
  The first results of a time dependent simulation of chromospheric
  response to a high energy electron beam are presented. The hybrid code,
  i.e. a combination of a 1-D hydrodynamic code and a test particle code,
  has been used to calculate the energy losses of a high energy electron
  beam propagating through the solar atmosphere and the consequent
  response of the ambient solar plasma to the energy deposition. The
  resulting time evolution of the solar plasma temperature, density,
  velocity and energy deposit on hydrogen has then been used as an input
  for a time dependent radiative transfer code in the MALI approach
  to determine the time variation of the Hα line profile. Non-thermal
  collisional rates have been included in the linearised ESE.

---------------------------------------------------------
Title: A prominence with transition region: horizontal two-dimensional
    filament model
Authors: Gorshkov, A. B.; Anzer, U.; Heinzel, P.
2002ESASP.506..405G    Altcode: 2002ESPM...10..405G; 2002svco.conf..405G
  SOHO/SUMER observations of solar filaments in Lyman lines of hydrogen
  have revealed, in general, a two-peak form of the emission line
  profiles with peak to center ratio less than an order of magnitude. This
  fact strongly contradicts the results of numerical radiative transfer
  simulations, where profiles with strong dips and large (1.5-2 orders of
  magnitude) peak to center ratio are usually obtained due to the absence
  of incident radiation from above the filament and, as a consequence,
  very low atomic populations on the upper energy levels at the top of
  the filament. Recently it was shown (Schmieder et al. 1998) that this
  discrepancy can be removed by introducing a prominence-corona transition
  region (PCTR) to the radiative transfer models. This paper continues
  a set of publications (Anzer &amp; Heinzel, 1999 and Heinzel &amp;
  Anzer, 2001) devoted to the modelling of prominences as structures in
  MHS equilibrium. Here the prominence is represented by a horizontal
  2D slab supported by a magnetic field. In our model we use a constant
  gas pressure and assume that the kinetic temperature profile and the
  PCTR extension are different in the vertical and horizontal directions
  due to magnetic field. In the PCTR the temperature sharply increases
  outwards from 8000K to 50000K on the scale of 100-600 km. To solve
  the radiative transfer problem we apply a 2D code based on the MALI
  iteration scheme and the modified long characteristics method.

---------------------------------------------------------
Title: Soft X-ray heating of the solar chromosphere: gradual phase
    of a solar flare
Authors: Berlicki, A.; Heinzel, P.; Jakimiec, J.
2002ESASP.506..549B    Altcode: 2002svco.conf..549B; 2002ESPM...10..549B
  In this paper we present the analysis of energetics of solar flaring
  chromosphere heated by soft X-ray radiation coming from overlying
  hot flare loops. During the solar flare, a large amount of its energy
  is emitted from hot coronal part in soft X-ray spectral range. This
  radiation can penetrate into the chromosphere and transmit the
  energy. This additional heating modifies vertical structure of the
  chromosphere and it can cause the enhanced emission from some parts of
  the flare. Therefore, such a mechanism can be responsible for emission
  of chromospheric flaring structures commonly observed in Hα and other
  spectral lines during the gradual phases when non-thermal processes
  are unimportant. To analyze the effect of X-ray heating we used the
  observations of the solar flare of 25 September 1997. This flare
  was observed with the Wroclaw Multichannel Subtractive Double Pass
  spectrograph (MSDP) coupled with the Large Coronagraph. We also use
  X-ray observations of the flare taken with the SXT telescope. Within
  the approximation of the quasi steady-state we have calculated the
  deposit of X-ray energy in the chromosphere. By means of the non-LTE
  radiative transfer calculations we show that enhanced emission of some
  H-alpha structures observed during the gradual phase of this solar
  flare can be partially explained in terms of the soft X-ray heating of
  the chromosphere by hot 'post-flare' loops seen on the SXT images. We
  also analyzed the energy budget of X-ray heated flaring chromosphere
  and found that radiative losses from the chromosphere can be balanced
  by soft X-ray heating only in some layers of the solar chromosphere.

---------------------------------------------------------
Title: Line profiles and intensity ratios in prominence models with
    a prominence to corona interface
Authors: Labrosse, N.; Gouttebroze, P.; Heinzel, P.; Vial, J. -C.
2002ESASP.506..451L    Altcode: 2002svco.conf..451L; 2002ESPM...10..451L
  In this work we study the hydrogen, helium and calcium spectra
  emitted by a one-dimensional prominence model in magneto-hydrostatic
  equilibrium. The prominence slab consists of two parts: a cool
  core where the plasma is optically thick for some lines, and a
  prominence-to-corona transition region (PCTR) with a strong temperature
  gradient. The models are defined by 5 parameters: temperature, pressure,
  slab thickness, microturbulent velocity and altitude. We solve the NLTE
  radiative transfer equations for all optically thick transitions. We
  present line ratios between infrared, optical and EUV lines, as well
  as line profiles. We show that the presence of a PCTR, where both
  collisional and radiative excitations are important, affects H, He,
  and Ca populations and emergent lines in different manners.

---------------------------------------------------------
Title: Spectral diagnostics of the magnetic field orientation in a
    round-shaped filament
Authors: Schmieder, B.; Mein, N.; Heinzel, P.; Anzer, U.
2002ESASP.506..469S    Altcode: 2002ESPM...10..469S; 2002svco.conf..469S
  During several campaigns focused on prominences we have obtained
  coordinated spectral observations from the ground and from space. The
  SOHO/SUMER spectrometer allows us to observe, among others, the whole
  Lyman series of hydrogen, while the Hα line was observed by the MSDP
  spectrograph at the VTT. For Lyman lines, the non-LTE radiative-transfer
  computations have shown the importance of the prominence-corona
  transition region (PCTR) and its relation to the magnetic field
  orientation for the explanation of the observed line profiles (Schmieder
  et al. 1998, Heinzel et al. 2001). Moreover, Heinzel and Anzer (2001)
  developed new 2D models which demonstrate how the shapes of Lyman
  lines vary depending on the orientation of the magnetic field with
  respect to the line of sight. To confirm this result observationally,
  we focus here on a round-shaped filament observed during three days
  as it was crossing the limb. The Lyman profiles observed on the limb
  are different from day to day and we interpret these differences by
  the change of orientation of the prominence axis (and therefore the
  magnetic field direction) with respect to the line-of-sight.

---------------------------------------------------------
Title: Prediction of line intensity ratios in solar prominences
Authors: Gouttebroze, P.; Labrosse, N.; Heinzel, P.; Vial, J. -C.
2002ESASP.505..421G    Altcode: 2002solm.conf..421G; 2002IAUCo.188..421G
  Solar prominences are made of relatively cool and dense plasma
  embedded in the solar corona, supported and structured by the magnetic
  field. Since this plasma is definitely out of LTE, the diagnosis
  of physical conditions in prominences needs the use of specific
  radiative transfer (RT) codes to predict the spectrum emitted by
  models and compare it to observations. For optically thin lines, the
  solution of RT equations in the transition itself is not required,
  but the emitted intensities depend, via the statistical equilibrium
  equations, on RT in other transitions which are optically thick. We
  use two different sets of models. The first one contains monolithic
  models defined by 5 parameters: temperature, pressure, thickness,
  microturbulent velocity and altitude above the solar surface. For
  each parameter, we assume a range of variation. For each model, the
  values of the 5 parameters are randomly chosen within the corresponding
  range of variation. The second set contains composite models made of
  multiple layers, in order to simulate the penetration of radiation into
  inhomogeneous prominences. We use NLTE radiative transfer codes to
  compute the intensities of the lines of hydrogen, helium and calcium
  emitted by each model. So, for any couple of lines, we may obtained
  their intensity ratio as a function of the 5 parameters. We discuss
  the behaviour of some of these intensity ratios as a function of the
  principal parameters and construct distribution diagrams, which are
  compared to different published observations.

---------------------------------------------------------
Title: Calcium to hydrogen line ratios in solar prominences
Authors: Gouttebroze, P.; Heinzel, P.
2002A&A...385..273G    Altcode:
  The ratio of Ca II 8542 Å to Hβ line intensities has been used for a
  long time to diagnose the gas pressure in solar prominences. In this
  paper we reconsider the theoretical dependence of E(8542)/E(Hβ ) on
  the gas pressure, as originally computed by Heasley &amp; Milkey (1978),
  and extend this theoretical correlation to higher pressures. Firstly, we
  revise the formation of calcium lines in prominences, using in parallel
  two independently developed NLTE radiative transfer codes. Computations
  consist of two subsequent steps: (i) the formation of hydrogen spectrum
  (treated in a similar way as in Gouttebroze et al. 1993), and (ii)
  the formation of calcium lines, using the electron-density structure
  obtained in step (i). The influence of hydrogen Lyman lines on Ca II to
  Ca III ionization is found to be very important for the determination
  of calcium-to-hydrogen line ratios. In particular, the intensities
  obtained for calcium lines at low pressures are significantly lower than
  those obtained by Heasley &amp; Milkey (1978), which is the result
  of a greater Ca III/Ca II ratio. Our numerical results have been
  further checked against an approximate analytical model. Secondly,
  we have performed an extended computation using a large grid of
  models covering different temperatures, gas pressures, geometrical
  thicknesses, microturbulent velocities and prominence altitudes. For
  temperatures lower than 10 000 K and pressures lower than 0.1 dyn
  cm<SUP>-2</SUP>, the line ratio E(8542)/E(Hβ ) undergoes only small
  variations, remaining between 0.2 and 0.3. At higher pressures (0.1
  to 1 dyn cm<SUP>-2</SUP>), the behaviour of this ratio appears to be
  strongly dependent on temperature: rapidly increasing below 6000 K,
  moderately increasing between 6000 and 8000 K, and generally decreasing
  at higher temperatures. A comparison of the present models with recent
  observations of Stellmacher &amp; Wiehr (2000) suggests the existence
  of cool prominence structures with temperatures around 6000 K and gas
  pressures higher than 0.1 dyn cm<SUP>-2</SUP>.

---------------------------------------------------------
Title: Theoretical hydrogen population relations for horizontal
    cloud-like solar structures
Authors: Tziotziou, K.; Mein, N.; Mein, P.; Heinzel, P.
2002ESASP.477..183T    Altcode: 2002scsw.conf..183T
  A large set of parameterized NLTE models has been computed for a 1D
  horizontal cloud-like structure standing above the solar surface. The
  used input model parameters are temperature, velocity, microturbulence,
  electronic density and geometrical thickness of the structure. From
  the output of our computations which is the hydrogen level populations
  as a function of the line center optical depth, we calculate several
  relations between the hydrogen population levels and the considered
  electron density. These relations are important for the study of
  prominence-like structures from observations.

---------------------------------------------------------
Title: Diagnostics of electron bombardment in solar flares from
    hydrogen Balmer lines
Authors: Kašparová, J.; Heinzel, P.
2002A&A...382..688K    Altcode:
  Influence of non-thermal collisional rates, related to an electron
  beam, on hydrogen Balmer line profiles is investigated. Semi-empirical
  temperature structure of the flare model F1 has been used for computing
  non-LTE profiles of Hα , Hβ , and Hγ . Contribution functions
  and their change due to different values of beam parameters are
  shown. Unlike the line core intensity, the intensity of line wings
  considerably depends on beam parameters and it is significantly
  enhanced for typical values of the beam energy flux. The ratio of
  line intensities at a selected wavelength is proposed to be used for
  diagnostics of electron beams during solar flares, particularly at
  impulsive phases. Obtained Hα line profiles are compared to those of
  Fang et al. (\cite{fhg93}).

---------------------------------------------------------
Title: Understanding solar flares from optical observations
Authors: Heinzel, P.
2002cosp...34E1097H    Altcode: 2002cosp.meetE1097H
  During the impulsive phase of solar flares, both hard X-ray (HXR) and
  optical emissions exhibit fast temporal fluctuations detectable down to
  sub-second scales. This is usually ascribed to the propagation of beams
  of accelerated particles and to the dissipation of their energy in lower
  layers of the solar atmosphere. Although it is rather difficult to prove
  a temporal correlation between HXR and optical intensity variations,
  we discuss here some previous results and recent attempts. Namely
  in coordination with RHESSI observations, several GBO's started to
  detect fast optical variations in the H-alpha line. In addition to
  this, we also explore a possibility of using some other diagnostically
  relevant lines. The proper interpretation of coordinated HXR and optical
  observations further requires robust tools for radiation-hydrodynamical
  (RHD) forward modeling. We briefly describe a new 'hybrid' code which
  consists of RHD part and particle-simulation part. Short-duration beam
  heating (pulses) is modeled and we predict temporal fluctuations of HXR
  and selected optical and UV lines formed in chromospheric layers and in
  the transition region. Particularly the line asymmetries originating
  in a highly dynamical lower atmosphere of the flare can be used to
  diagnose the response of these layers to particle beams.

---------------------------------------------------------
Title: Why Are Solar Filaments More Extended in Extreme-Ultraviolet
    Lines than in Hα?
Authors: Heinzel, P.; Schmieder, B.; Tziotziou, K.
2001ApJ...561L.223H    Altcode:
  A long solar filament was observed simultaneously in the Hα line
  by THEMIS/MSDP and in selected EUV lines by the Coronal Diagnostic
  Spectrometer on SOHO. Co-alignment of optical and EUV images reveals
  that the dark EUV filament is much more extended than the Hα
  filament. Assuming that the EUV filament represents Lyman continuum
  absorption of the background EUV-line radiation, a straightforward
  explanation of this effect is suggested. Based on non-LTE filament
  models, we demonstrate that the ratio of the Lyman continuum to Hα
  opacity can reach a factor of 50-100, and thus the EUV filament is
  still well visible while the Hα line contrast diminishes below the
  detection limit. This kind of interpretation leads to an important
  conclusion that the cool filament material in which the Lyman continuum
  absorption takes place is more abundant than one would expect from
  Hα disk observations. This then may have significant consequences
  on the filament structure and on formation models, as well as on mass
  considerations related to coronal mass ejections.

---------------------------------------------------------
Title: Prominence fine structures in a magnetic equilibrium:
    Two-dimensional models with multilevel radiative transfer
Authors: Heinzel, P.; Anzer, U.
2001A&A...375.1082H    Altcode:
  In this paper we construct theoretical models for vertical prominence
  threads which are in magnetohydrostatic (MHS) equilibrium. These
  models are fully two-dimensional (2D) and take the form of vertically
  infinite threads hanging in a horizontal magnetic field. A typical
  example of such a 2D magnetic-dip structure is shown for the case
  when the central cool parts are surrounded by the prominence-corona
  transition region (PCTR). We display 2D variations of the pressure,
  density and temperature. While the pressure variations follow from the
  MHS equilibrium, the kinetic temperature was specified empirically. As a
  next step, we have solved the 2D multilevel non-LTE transfer problem in
  such thread-like structures, in order to predict the spatial variations
  of the emergent hydrogen spectrum. It is demonstrated that the hydrogen
  Lyman lines (treated with partial redistribution) show significant
  spatial variations of the intensity and that an important difference
  exists between the line profiles emergent along and across the magnetic
  field lines. We also discuss how these intensity variations compare to
  recent SOHO/SUMER prominence observations, namely we show the effects
  of line-profile averaging over the fine-structure threads which are
  below the instrumental resolution. Finally we make some suggestions
  for future modelling and observations.

---------------------------------------------------------
Title: A Study of Hydrogen Density in Emerging Flux Loops from
    a Coordinated Transition Region and Coronal Explorer and Canary
    Islands Observation Campaign
Authors: Mein, N.; Schmieder, B.; DeLuca, E. E.; Heinzel, P.; Mein,
   P.; Malherbe, J. M.; Staiger, J.
2001ApJ...556..438M    Altcode:
  During an international ground-based campaign in the Canary Islands
  coordinated with space instruments (i.e., Transition Region and Coronal
  Explorer [TRACE]), we observed an active region on 1998 September
  10 with high spatial and temporal resolution. New emerging flux in
  the central part of the active region was observed in magnetograms
  of the Swedish Vacuum Solar Telescope, La Palma. Emerging loops
  (arch-filament systems [AFSs]) are well developed in Hα and Ca II
  according to the observations made at the Vacuum Tower Telescope (VTT)
  and THEMIS telescope in Tenerife with the Multichannel Subtractive
  Double Pass (MSDP) spectrographs. The TRACE images obtained at 171
  and 195 Å show low-emission regions that are easily identified as
  the individual AFS. They are due to absorption by hydrogen and helium
  continua in the cool filament plasma. We compare two techniques of
  measuring the hydrogen density in the cool dense fibrils of AFSs. The
  first method based on TRACE observations derived the neutral hydrogen
  column density of the plasma absorbing coronal lines. The second one
  using Hα line profiles provided by the MSDP spectrographs is based on
  the cloud model. The results are consistent. We derive also electron
  density values using Hα lines that are in good agreement with those
  derived from the 8542 Å Ca II line observed with THEMIS (Mein et
  al.). The three types of observations (TRACE, VTT, THEMIS) are well
  complementary: absorption of coronal lines giving a good approximation
  for the maximum value of the neutral hydrogen column density, the Hα
  line giving a good determination of n<SUB>e</SUB>, and the 8542 Å Ca
  II line a good determination of the electronic temperature.

---------------------------------------------------------
Title: SOHO/SUMER observations and analysis of the hydrogen Lyman
    spectrum in solar prominences
Authors: Heinzel, P.; Schmieder, B.; Vial, J. -C.; Kotrč, P.
2001A&A...370..281H    Altcode:
  The complete hydrogen Lyman spectrum in several prominences has been
  observed with the UV spectrometer SUMER on-board the SOHO, during
  the Joint Observing Programme 107, together with other space and
  ground-based observatories. Based on these observations, we are able to
  demonstrate, for the first time, that there exists a large variety of
  intensities and shapes of Lyman lines in different prominences and in
  various parts thereof. Therefore, no “canonical” Lyman spectrum can
  be considered for modelling purposes. However, we have identified at
  least two representative properties of the observed spectra: in one case
  (May 28, 1999 prominence) we detected high integrated intensities and
  no reversals in lines higher than Lalpha . Another prominence (June 2,
  1999) exhibited quite similar integrated intensities, but all lines have
  rather strongly reversed profiles. This behaviour cannot be explained in
  terms of standard isothermal-isobaric models and we thus consider more
  general models which are in pressure equilibrium with the magnetic field
  and which have significant prominence-corona transition region (PCTR)
  temperature gradients. This type of model, recently suggested by Anzer
  &amp; Heinzel (\cite{anhe99}), is capable of explaining strong emission
  profiles without reversal. Based on extended non-LTE computations,
  we suggest that quite different Lyman spectra mentioned above may
  correspond to two types of PCTRs, one seen along the magnetic-field
  lines (unreversed profiles) and the other one seen across the field
  lines (reversed profiles). Finally, we again confirm the importance
  of partial-redistribution (PRD) scattering processes for Lyman lines
  in prominences. However, our analysis of new SUMER data also points
  to a critical role of the PCTR in radiative transport in these lines.

---------------------------------------------------------
Title: Non-LTE inversion of chromospheric {\Ca Ii} cloud-like features
Authors: Tziotziou, K.; Heinzel, P.; Mein, P.; Mein, N.
2001A&A...366..686T    Altcode:
  A chromospheric cloud-like feature observed in the 8542 Å {{Ca Ii}
  line is studied by a two step inversion procedure which provides
  estimates of its temperature, electronic density, microturbulence,
  geometrical thickness and bulk velocity. The first step involves the
  computation of a large grid of models by a multi-level non-LTE transfer
  code which gives the {{Ca Ii} line depth-dependent mean intensity
  inside an isolated, isothermal cloud lying above the chromosphere. The
  second step involves the inversion of the observed profiles with the
  grid of computed synthetic {{Ca Ii} profiles. A searching and matching
  chi <SUP>2</SUP> algorithm is implemented followed by an interpolation
  algorithm which permits a more accurate determination of the parameters
  on which the profiles depend. The five grid parameters are reduced to
  four by defining the emission measure from the geometrical thickness
  and electronic density. We show that this inversion procedure gives
  accurate results for some of our inversion parameters when dealing
  with solar filaments and is complementary to a previous study of the
  same object in the {{Hα }} line. The main advantages, problems and
  future extension of the inversion approach are also discussed.

---------------------------------------------------------
Title: Simultaneous SOHO and Ground-Based Observations of a Large
    Eruptive Prominence and Coronal Mass Ejection
Authors: Plunkett, S. P.; Vourlidas, A.; Šimberová, S.; Karlický,
   M.; Kotrč, P.; Heinzel, P.; Kupryakov, Yu. A.; Guo, W. P.; Wu, S. T.
2000SoPh..194..371P    Altcode:
  Coronal mass ejections (CMEs) are frequently associated with
  erupting prominences near the solar surface. A spectacular eruption
  of the southern polar crown prominence was observed on 2 June 1998,
  accompanied by a CME that was well-observed by the LASCO coronagraphs
  on SOHO. The prominence was observed in its quiescent state and was
  followed throughout its eruption by the SOHO EIT and later by LASCO
  as the bright, twisted core of the CME. Ground-based Hα observations
  of the prominence were obtained at the Ondřejov Observatory in the
  Czech Republic. A great deal of fine structure was observed within
  the prominence as it erupted. The prominence motion was found to
  rotate about its axis as it moved outward. The CME contained a helical
  structure that is consistent with the ejection of a magnetic flux rope
  from the Sun. Similar structures have been observed by LASCO in many
  other CMEs. The relationship of the flux rope to other structures in
  the CME is often not clear. In this event, the prominence clearly lies
  near the trailing edge of the structure identified as a flux rope. This
  structure can be observed from the onset of the CME in the low corona
  all the way out to the edge of the LASCO field of view. The initiation
  and evolution of the CME are modeled using a fully self-consistent,
  3D axisymmetric, MHD code.

---------------------------------------------------------
Title: Energy considerations for solar prominences with mass inflow
Authors: Anzer, U.; Heinzel, P.
2000A&A...358L..75A    Altcode:
  In this Letter we study the inflow of enthalpy and ionisation
  energy into solar prominences. We use 1D stationary slab models for
  the prominence to calculate this inflow. We compare the resulting
  energy gain with the integrated radiative losses obtained for such
  slab models. We find that for reasonable inflow velocities many of our
  models can be in energy equilibrium; only the very massive prominences
  will either require some additional heating or they have to cool down
  to low central temperatures. We also discuss the possibility or heating
  the prominence by vertical downflows.

---------------------------------------------------------
Title: Decaying post-flare loops system observed by SOHO/CDS and
    Yohkoh/SXT
Authors: Varady, M.; Fludra, A.; Heinzel, P.
2000A&A...355..769V    Altcode:
  The results of an analysis of joint SOHO/CDS and Yohkoh/SXT observations
  of a decaying post-flare loops system with a rapid time evolution are
  presented. The loop system was a remnant of a small single loop flare
  (GOES class C2.9). Using the CDS raster taken in several EUV lines with
  different formation temperatures and a temperature sensitive line pair
  Fe XVI 360.8/Si XII 520.7 we confirmed the existence of the vertical
  stratification in the loop system according to the line formation
  temperature. The analysis of the SXT data showed a strong decay of the
  system with time. While the temperature of the hot part of the system
  (T =~ 2.5 MK) decreased only slightly, the total emission measure
  dropped by more than a factor of four in approximately 10<SUP>3</SUP>
  s. This could be explained by a plasma outflow from the loops with
  velocity approximately 10 km/s. On the other hand, signs of rapid,
  probably radiative cooling can be identified in the images obtained
  from the CDS raster taken in cool lines of O V and O III. Using the
  density sensitive line pair of Fe XIV 334.2/353.8 and the integrated
  intensity of Fe XIV 334.2 line we determined the electron densities
  and emission measures across the top of the loop system. From the
  results of these measurements, taking all known uncertainties into
  account, we obtained that the geometrical filling factor at the top of
  the system in the regions with maximum electron density in the Fe XIV
  line lies in the interval from =~ 0.01 to =~ 0.2. A simple theoretical
  approximation of the energy balance in the post-flare plasma gives a
  total cooling time =~ 750 s.

---------------------------------------------------------
Title: Solar arch filaments observed with THEMIS
Authors: Mein, P.; Briand, C.; Heinzel, P.; Mein, N.
2000A&A...355.1146M    Altcode:
  Arch Filaments (AF) have been observed in the Ca Ii 8542 Å line with
  the THEMIS telescope in September 1998. We present a preliminary
  analysis of MSDP spectro-imaging data. A cloud-model fit provides
  line-of-sight velocities and a set of plausible values for the model
  parameters. The high sensitivity of the filament opacity to temperature,
  coupled with the rough linearity versus electronic density, shows that
  this Ca Ii line should be very efficient to complement usual Hα data
  for a more rigorous diagnostics. Based on observations made with the
  THEMIS telescope operated on the island of Tenerife by CNRS-CNR in
  the spanish Observatorio del Teide of the Instituto de Astrofisica
  de Canarias

---------------------------------------------------------
Title: Study of Chromospheric Ca II Cloud-like Structures
Authors: Tziotziou, K.; Heinzel, P.; Mein, P.; Mein, N.
2000ESASP.463..443T    Altcode: 2000sctc.proc..443T
  No abstract at ADS

---------------------------------------------------------
Title: Commission 12: Solar Radiation and Structure (Radiation et
    Structure Solaires)
Authors: Foukal, Peter; Solanki, Sami; Mariska, J.; Baliunas, S.;
   Dravins, D.; Duvall, T.; Fang, C.; Gaizauskas, V.; Heinzel, P.;
   Kononovich, E.; Koutchmy, S.; Melrose, D.; Stix, M.; Suematsu, Y.;
   Deubner, F.
2000IAUTA..24...73F    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Models of the solar atmosphere
Authors: Heinzel, P.
2000ASIC..558..201H    Altcode: 2000asre.conf..201H
  Contents: Basic equations of radiation hydrodynamics. Solution of
  NLTE problems. Semiempirical models of the solar atmosphere. Dynamical
  models.

---------------------------------------------------------
Title: Phase Relations between Chromospheric and Transition Region
    Oscillations
Authors: Krijger, J. M.; Curdt, W.; Heinzel, P.; Schmidt, W.
2000ESASP.463..353K    Altcode: 2000sctc.proc..353K
  No abstract at ADS

---------------------------------------------------------
Title: Solar Prominences Observed by Soho (SUMER, CDS, EIT) and
    Ground-Based Observatories (GBO)
Authors: Heinzel, P.; Schmieder, B.; Vial, J. C.; Rudawy, P.
2000AdSpR..25.1777H    Altcode:
  We present two sets of prominence observations in higher lines
  of the hydrogen Lyman series (from Lδ to L-9), together with
  some other UV lines. These data have been obtained by the Solar
  Ultraviolet Measurements of Emitted Radiation (SUMER) onboard the
  SOHO satellite in June 1997. Coordinated observations were also taken
  by other SOHO instruments: Coronal Diagnostic Spectrometer (CDS) and
  Extreme-Ultraviolet Imaging Telescope(EIT) and with the coronagraph
  of the Wroclaw University Observatory at Bialkóv, the spectrograph
  of the Ondřejov Observatory. We demonstrate the basic characteristics
  of the calibrated line profiles and compare them with the theoretical
  profiles computed from isothermal-isobaric models

---------------------------------------------------------
Title: Chromospheric Response to a Short-Duration Beam Heating:
    Observing Programme and Numerical Simulations
Authors: Heinzel, P.; Karlický, M.; Kotrč, P.; Kupryakov, Yu. A.
2000ASPC..206..289H    Altcode: 2000hesp.conf..289H
  No abstract at ADS

---------------------------------------------------------
Title: Diagnostics Constraints on Prominence Parameters from SOHO
    and Ground-based Observations
Authors: Schmieder, B.; Kotrč, P.; Heinzel, P.; Kucera, T.;
   Andretta, V.
1999ESASP.448..439S    Altcode: 1999ESPM....9..439S; 1999mfsp.conf..439S
  No abstract at ADS

---------------------------------------------------------
Title: Simultaneous Observations of Chromospheric and Transition
    Region Oscillations in HI Lyman Transitions and in Optical Lines
Authors: Curdt, W.; Heinzel, P.; Schmidt, W.; Tarbell, T.; von
   Uexküll, M.; Wilken, V.
1999ESASP.448..177C    Altcode: 1999mfsp.conf..177C; 1999ESPM....9..177C
  No abstract at ADS

---------------------------------------------------------
Title: Decaying Post-Flare Loops System Observed By SOHO/CDS And
    Yohkoh/SXT
Authors: Varady, M.; Fludra, A.; Heinzel, P.
1999ESASP.446..669V    Altcode: 1999soho....8..669V
  The results of an analysis of joint CDS of SOHO and SXT of Yohkoh
  observations of a decaying post-flare loop system are presented. The SXT
  images were used to explain some peculiar structural features visible
  in the examined CDS raster, resulting from the rapid evolution of the
  observed system and from the way the CDS rasters are built. The SXT
  data was also used to determine the time evolution of the temperature
  and the emission measure of the hot part of the system during its
  decay. The CDS data, with a very good temperature coverage, contains
  a density sensitive line pair of Fe XIV which was used for electron
  density analysis and a temperature sensitive line pair of Fe XVI and
  Si XII which was used to study the temperature structure of the loop
  system. From the integrated intensities of selected lines the emission
  measures were calculated. From these measurements we estimated the
  filling factor of the loop system in Fe XIV line.

---------------------------------------------------------
Title: Hydrogen Lyman Lines and Continuum Emission in a Polar-Crown
    Prominence Observed with SUMER/SOHO
Authors: Schmieder, B.; Kucera, T.; Heinzel, P.; Vial, J. -C.
1999ESASP.446..605S    Altcode: 1999soho....8..605S
  We present, for the first time, a quasi-simultaneous spectroscopic
  observation of the whole Lyman series of HI and continuum in a
  quiescent prominence. Namely we have extended our previous study of
  higher Lyman lines to lower members of the series, particularly
  L-alpha and L-beta. For the latter two lines, we compare our
  calibrated profiles (free of geocoronal absorption) with previous
  data from OSO-8 LPSP spectrometer and (for L-alpha) from UVSP/SMM. We
  demonstrate the importance of Lyman lines for studies of the base of
  the prominence-corona transition region.

---------------------------------------------------------
Title: SOHO/SUMER observations and analysis of hydrogen Lyman lines
    in a quiescent prominence
Authors: Schmieder, B.; Heinzel, P.; Vial, J. C.; Rudawy, P.
1999SoPh..189..109S    Altcode:
  A quiescent prominence was observed in June 1997 by instruments
  onboard the SOHO spacecraft: the Solar Ultraviolet Measurements of
  Emitted Radiation (SUMER), Coronal Diagnostic Spectrometer (CDS)
  and Extreme-Ultraviolet Imaging Telescope (EIT), along with the
  coronagraph of the Wrocław University Observatory at Bialków and
  the spectrograph of the Ondřejov Observatory. We present prominence
  observations in higher lines of the hydrogen Lyman series (from Lδ
  to L-9), together with some other UV lines obtained by SUMER. We
  extract the basic characteristics of the calibrated line profiles
  of these Lyman lines and compare them with the theoretical profiles
  computed from three kinds of NLTE models which also include prominence
  filamentation. Our principal result is that the current NLTE models are
  in principle capable of explaining the SUMER calibrated intensities
  in the observed Lyman lines. We also find that in order to fit all
  these lines, one has to consider a prominence-corona transition region
  (PCTR) with a temperature gradient. At low pressures, higher Lyman
  lines are still rather sensitive to the incident radiation which must
  be carefully taken into account in the modeling. From PCTR models,
  which also take into account the effect of ambipolar diffusion on the
  heating, we have derived the formation depths for the Lyman series
  lines. High Lyman lines seem to be formed just at the base of the PCTR.

---------------------------------------------------------
Title: Coordinated Prominence Observations by SOHO and Ground-Based
    Observatories
Authors: Schmieder, B.; Heinzel, P.; Vial, J. -C.; Malherbe, J. M.;
   Mein, P.; Rudawy, P.; Ceppatelli, G.
1999ASPC..184..296S    Altcode:
  Coordinated observations obtained during the JOP12 (Joint Observing
  Programme between SOHO and ground-based instruments) allow us to
  analyse the physical conditions in a prominence of 5 June 1997 and
  its environment in the solar corona. The arch-shaped prominence shows
  either vertical or horizontal structures according to the observed
  lines (Hα with the coronagraph of the Wroclaw University Observatory
  at Bialków and lines in a broad temperature range by the Coronal
  Diagnostic Spectrometer CDS). The less dynamic behaviour of this
  prominence was shown by the persistence of bubbles in the prominence
  and confirmed by the Dopplershifts measured in CDS lines and in Hα
  by the Italian Panoramic Monochromator (IPM) filter on the THEMIS
  telescope in Tenerife. We explain the complex morphology of this
  prominence by recent 3D MHD models. Finally, we present prominence
  spectra in higher lines of the hydrogen Lyman series (from Lδ to L-9),
  together with some other UV lines. These data have been obtained by
  the Solar Ultraviolet Measurements of Emitted Radiation (SUMER). We
  demonstrate the basic characteristics of the calibrated line profiles
  of Lyman lines and compare them with the theoretical profiles computed
  from isothermal-isobaric models. This leads to some constraints on
  the environment of the prominence.

---------------------------------------------------------
Title: Chromospheric Oscillations Observed by SUMER/SOHO
Authors: Heinzel, P.; Curdt, W.
1999ASPC..184..201H    Altcode:
  We discuss first observations of the temporal behaviour of the hydrogen
  Lyman lines made by the SUMER/SOHO spectrometer. Using the Ly 5 line,
  we show here the global oscillatory pattern of the whole line profile
  for three representative quiet-Sun structures: cell interior, network
  boundary, and bright network. Mean power spectra for these structures
  show several maxima, some of which are quite well correlated with the
  maxima derived from Ca II K_2V observations. In the cell interior, the
  power peak is centred between 4.5-5 mHz. No clear evidence of a 3 minute
  chromospheric mode was found. In the network, we observe a broad range
  of frequencies, with a maximum between 2-3 mHz. Lyman lines exhibit
  certain Doppler shifts and asymmetries, but the oscillatory behaviour is
  mainly due to the intensity variations which are small compared to the
  line intensity itself (they reach 10-20 % of the mean line intensity).

---------------------------------------------------------
Title: The energy balance in solar prominences
Authors: Anzer, U.; Heinzel, P.
1999A&A...349..974A    Altcode:
  In this paper we study the energy balance in quiescent solar
  prominences. For this investigation we use a simple 1D slab model in
  magneto-hydrostatic equilibrium. We divide the studied region into two
  parts: The inner region consisting of the prominence itself and the
  cool part of the transition region (up to 30000 K). In this region the
  plasma is optically thick in several atomic transitions and therefore we
  have to solve the non-LTE radiative transfer problem in this part. This
  allows us to derive self-consistently the gas density, the ionization
  degree of hydrogen and the hydrogenic radiation losses. The energy
  transport by thermal conduction can be neglected in this region. In the
  outer part of the transition region, the thermal conduction becomes very
  important but the treatment of radiation is simplified by the fact that
  the plasma is optically thin. We find that energy balance in prominences
  can only be obtained for special forms of the heating function. This
  requirement is very stringent for the inner parts, while in the outer
  region thermal conduction can transport large amounts of the heat
  energy and therefore a wider class of heating functions will be allowed.

---------------------------------------------------------
Title: Proton and hydrogen temperatures at the base of the solar
    polar corona
Authors: Marsch, E.; Tu, C. -Y.; Heinzel, P.; Wilhelm, K.; Curdt, W.
1999A&A...347..676M    Altcode:
  The SUMER (Solar Ultraviolet Measurements of Emitted Radiation)
  Spectrometer on SOHO (Solar and Heliospheric Observatory) has been
  used to observe the lines of the Lyman series (up to quantum numbers
  larger than 20) of hydrogen emitted in the solar atmosphere. The
  line shapes and intensities versus height are obtained near the limb
  from about -10\arcsec to 70\arcsec. The lines are broad and show the
  typical self-absorption reversal near the limb, where the emission
  comes from optically thick material, and change systematically with
  increasing height. The H i Ly6, Ly7 and Ly9 lines attain a Gaussian
  shape at heights above the visible limb between about 19\arcsec and
  22\arcsec, where the emission comes from an optically thin plasma. The
  line shapes and intensities can be fitted well by model profiles
  obtained from multilevel NLTE (Non Local-Thermodynamic-Equilibrium)
  radiative transfer calculations which allow us, assuming excitation
  and ionization equilibrium, to derive consistently the temperatures and
  densities of the hydrogen atoms and, with additional assumptions, of the
  protons. Temperature values range between 1 10(5) K to 2 10(5) K. We
  present the systematics of the line shapes as observed in different
  emission regions and discuss briefly the relevance of these results
  for the solar wind acceleration and coronal heating.

---------------------------------------------------------
Title: Cloud model with variable source function for solar Hα
    structures. II. Dynamical models
Authors: Heinzel, P.; Mein, N.; Mein, P.
1999A&A...346..322H    Altcode:
  It was demonstrated in the previous paper (Paper I)that the cloud
  model technique can be largely improved if one considers realistic
  boundary conditions in evaluating the true form of the line source
  function. For structures seen against the solar disk, the Hα line
  source function is decreasing from bottom towards the top. In the
  present paper we investigate the effect of Doppler brightening on Hα
  source function. In frame of 1D non-LTE models it is demonstrated how
  the Hα line source function is increased depending on the velocity
  of the moving cloud and direction of the motion. For the same set of
  cloud models as used in Paper I, we have reevaluated the variations of
  the source function with optical depth including the effect of cloud
  motion. The resulting curves have been approximated by a second-degree
  polynomial and the respective coefficients have been subsequently
  used in a modified iterative method in order to derive the cloud
  model parameters. As expected, dynamical models lead to more precise
  specification of these parameters, namely the optical thickness, as
  compared to the static case investigated in Paper I. We have applied
  this new method to MSDP observations of a dark chromospheric feature
  (loop) with considerable flows.

---------------------------------------------------------
Title: A non-LTE inversion procedure for chromospheric cloud-like
    features
Authors: Molowny-Horas, R.; Heinzel, P.; Mein, P.; Mein, N.
1999A&A...345..618M    Altcode:
  A fast inversion procedure which provides estimates of the temperature,
  electronic density, microturbulence, geometrical thickness and bulk
  velocity of chromospheric features, so-called “clouds”, has been
  implemented. The procedure has been divided into two steps: 1) the
  construction of a large grid of models by means of a multi-level non-LTE
  transfer code, which solves in a fast and reliable way the radiative
  transfer problem of the formation of the Hα line inside an isolated,
  isothermal cloud laying above the photosphere, and 2) the implementation
  of searching, matching and interpolating algorithms which yield an
  inversion of the observed line profile in terms of the grid's computed
  profiles. The aforementioned 5 parameters, on which the profiles depend,
  can be reduced to 4 if one defines the so-called emission measure from
  the geometrical thickness and electronic density parameters. We show
  that this strategy yields excellent results when dealing with solar
  filaments. The main advantages of this approach are also discussed.

---------------------------------------------------------
Title: Magnetic Dips in Prominences
Authors: Heinzel, P.; Anzer, U.
1999SoPh..184..103H    Altcode:
  Magnetic dips are generally assumed to be basic equilibrium
  configurations in quiescent solar prominences. Here we discuss two types
  of the magnetic dips which were considered in the literature: (1) dips
  resulting from a force-free magnetic equilibrium in the corona, and (2)
  magnetic dips which are formed in situations where the Lorentz force
  balances the weight of the prominence plasma. An important parameter
  which decides between these two cases is the plasma β. For β⋘1,
  the effect of the prominence material on the equilibrium structure is
  quite negligible and the case (1) holds. If, however, β is larger,
  say between 0.1 and 1 or even higher, magnetic dips of the second kind
  are formed and they can be characterized by the angle ψ1 between the
  vertical and the direction of the field lines at the surface of the
  prominence structure. A simple and illustratory formula is derived
  to relate this angle to the plasma β at the prominence center,
  namely βc≃cot2ψ1. βc=1 thus corresponds to ψ1=45°. Finally,
  we discuss the range of values of both βc and ψ1 as deduced from
  various observations and conclude that the dips of the second kind are
  important for the prominence equilibria. We also suggest a new method
  for determination of the field-line inclination.

---------------------------------------------------------
Title: Eruptive filament of May 31, 1997, observed by SOHO.
Authors: Schmieder, B.; Heinzel, P.; Vial, J. -C.; Delaboudinière,
   J. -P.; Delannée, C.
1999joso.proc..147S    Altcode:
  In the frame of the SUMER/CDS Joint Programme (JOP 17) the authors
  have detected the four Lyman lines in an erupting filament. The
  strong self-absorption in these lines, already reported for quiescent
  filaments, is still present in this highly dynamical event, but the
  authors observe a significant red asymmetry in the intensities of the
  two peaks. They ascribe it to an upward bulk motion of the filament,
  which they can actually see on a series of EIT images taken in the
  Fe XII line. Both sets of observations can lead to a determination
  of the velocity vector. The Doppler velocities are also derived from
  other lines detected by SUMER/CDS and can be correlated with the
  observations of the Pic-du-Midi MSDP obtained for this event. The
  filament eruption was also well observed by other GBO instruments in
  the Hα line (Meudon and Ondřejov).

---------------------------------------------------------
Title: Chromospheric Oscillations Observed by SOHO/SUMER and VTT/GCT
    on Tenerife
Authors: Curdt, W.; Heinzel, P.; Schmidt, W.; von Uexküll, M.;
   Wilken, V.
1999AGAb...15R..11C    Altcode: 1999AGM....15..A12C
  Previous studies have revealed various oscillations in higher Lyman
  lines of hydrogen, as observed with SUMER on SOHO (Curdt &amp; Heinzel
  1998). The assumption that these periodic phenomena might be related
  to similar effects observed in optical lines like Ca II K led to the
  idea of simultaneous observations with the SOHO/SUMER instrument and
  the VTT/GCT telescopes on Tenerife. First results are presented here
  for the Lyman series and Lyman continuum. Power spectra in network and
  internetwork regions have been derived and a preliminary interpretation
  based on the wave propagation concept is given. In SUMER spectra
  we found a well-pronounced asymmetry of all Lyman lines, which is
  related to atmospheric dynamics. The time variation of co-spatial UV
  and optical data is presented and basic characteristics are discussed.

---------------------------------------------------------
Title: Non-LTE inversions of solar filament in Hα profiles.
Authors: Molowny-Horas, R.; Mein, P.; Mein, N.; Heinzel, P.
1999joso.proc..209M    Altcode:
  Results are shown of a new grid-based, non-LTE inversion procedure
  which can carry out fast and accurate spectral inversions of Hα line
  profiles. The code has been applied to a set of observed MSDP Hα line
  profiles of a solar filament. The results of this inversion are shown
  as 2-D maps of temperature, microturbulence and emission measure.

---------------------------------------------------------
Title: Dynamic Behavior of the Upper Solar Atmosphere: Sumer/ Solar
    and Heliospheric Observatory Observations of Hydrogen Lyman Lines
Authors: Curdt, Werner; Heinzel, Petr
1998ApJ...503L..95C    Altcode:
  We present first observations of the temporal evolution of hydrogen
  Lyman lines, made by the Solar Ultraviolet Measurements of Emitted
  Radiation (SUMER) spectrometer on the Solar and Heliospheric
  Observatory. A time series of about 33 minutes was obtained on 1997
  June 5. The entrance slit has crossed a quiet-Sun region of 115.3" with
  two internetwork structures (cells) and the bright network regions. A
  data set of 59 spectra with30 s exposure time was obtained, using
  the SUMER tracking system to compensate for the solar rotation. For
  our analysis, we have selected a Lyman continuum window around 907
  Å and the three Lyman lines Ly5, Ly9, and Ly15, which are formed at
  different depths in the upper chromosphere. In the cell interiors,
  we have detected significant periodic intensity variations with a
  Fourier transform power peak at 3.3-3.5 minutes, which is consistent
  with 3 minute internetwork oscillations. They seem to be associated
  with spatially unresolved “clusters” of grains. In the bright network
  regions, we detect slower oscillations of 6.9-7.6 minutes. These waves
  seem to propagate upward as we deduce from a phase shift between the
  three Lyman lines studied. The phase velocity was estimated to be
  roughly 3 km s<SUP>-1</SUP> in the network. Finally, we discuss the
  potential usefulness of the hydrogen Lyman lines for diagnostics of the
  temperature structure of the upper solar atmosphere. Our observations,
  in particular the fact that we see all Lyman lines in emission all of
  the time, put certain constraints on the temperature gradients above
  the region in which numerical simulations do predict a decrease of
  the mean kinetic temperature.

---------------------------------------------------------
Title: Filament Observations with SOHO Sumer/cds: The Behaviour of
    Hydrogen Lyman Lines
Authors: Schmieder, B.; Heinzel, P.; Kucera, T.; Vial, J. -C.
1998SoPh..181..309S    Altcode:
  On 21 September 1996, a filament close to an area of enhanced network
  was observed with the Solar Ultraviolet Measurements of Emitted
  Radiation (SUMER) spectrometer and Coronal Diagnostic Spectrometer
  (CDS). CDS provided intensity, Doppler shift and linewidth maps of the
  region in six lines whose temperature range covers 10<SUP>4</SUP> to
  10<SUP>6</SUP> K. SUMER observations consisted of maps of the region
  in four hydrogen Lyman lines (Lδ, L∈, L-6, L-7) and a Svi line
  (944 Å). In all the Lyman lines we detect a central absorption
  and an asymmetry in the intensity of the two peaks. First NLTE
  computations indicate that such reversed Lyman profiles and their
  absolute intensities can be reproduced with the existing filament models
  provided that we take into account a prominence-corona transition region
  (PCTR). We discuss the Lyman lines' asymmetry in terms of macroscopic
  flows by comparison with the Hei line Doppler shifts observed with CDS.

---------------------------------------------------------
Title: Prominence Parameters Derived from Magnetic-Field Measurements
    and NLTE Diagnostics
Authors: Anzer, U.; Heinzel, P.
1998SoPh..179...75A    Altcode:
  In this paper we present a detailed analysis of a number of quiescent
  prominences for which the components of the magnetic field as well as
  the electron density and emission measure were previously obtained from
  quasi-simultaneous measurements in hydrogen Hα and helium D<SUB>3</SUB>
  lines. From magnetic equilibrium models of the Kippenhahn-Schlüter
  type one can calculate the gas pressure, density, column mass and
  geometrical width. The same set of physical parameters can also
  be derived from a NLTE hydrogen-line analysis. We have studied the
  mutual correlations between these two sets of parameters. Very large
  differences, reaching an order of magnitude, were found between these
  two sets, both for individual prominences and for the mean values over
  all prominences used in this investigation. Finally, we discuss some
  implications of our results.

---------------------------------------------------------
Title: Lyman Lines in Prominences and Filaments: NLTE
    ModellingStrategies
Authors: Heinzel, P.
1998ASPC..150..188H    Altcode: 1998IAUCo.167..188H; 1998npsp.conf..188H
  No abstract at ADS

---------------------------------------------------------
Title: SUMER/SOHO Filament Observations in Selected Lyman Lines
Authors: Schmieder, B.; Kucera, T.; Heinzel, P.; Vial, J. -C.
1998ASPC..150..205S    Altcode: 1998IAUCo.167..205S; 1998npsp.conf..205S
  No abstract at ADS

---------------------------------------------------------
Title: 2-D Radiative Transfer Simulations with Angle-Dependent
    Partial Frequency Redistribution
Authors: Gorshkov, A. B.; Heinzel, P.
1998ASPC..150..209G    Altcode: 1998IAUCo.167..209G; 1998npsp.conf..209G
  No abstract at ADS

---------------------------------------------------------
Title: XIVth consultation on solar physics : conference proceedings
Authors: Rompolt, B.; Jakimiec, J.; Heinzel, P.
1998PAICz..88.....R    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Modelling of Non-Uniform Prominence Slabs
Authors: Heinzel, P.; Anzer, U.
1998ASPC..150..213H    Altcode: 1998IAUCo.167..213H; 1998npsp.conf..213H
  No abstract at ADS

---------------------------------------------------------
Title: New Evidence of Chromospheric Evaporation
Authors: Kasparova, J.; Kotrc, P.; Heinzel, P.; Nikulin, I. F.;
   Rudawy, P.
1998ASPC..150..397K    Altcode: 1998IAUCo.167..397K; 1998npsp.conf..397K
  No abstract at ADS

---------------------------------------------------------
Title: Height variations of prominence plasma parameters
Authors: Kotrč , P.; Heinzel, P.; Vial, J. -C.; Rompolt, B.
1998PAICz..88..208K    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Problems in prominence NLTE modeling
Authors: Heinzel, P.
1998PAICz..88..195H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Filament observations with SOHO SUMER/CDS.
Authors: Schmieder, B.; Kučera, T.; Heinzel, P.; Vial, J. -C.
1998joso.proc..136S    Altcode:
  During a coordinated campaign between SOHO and ground-based instruments
  a filament located close to the central meridian has been the target
  of SUMER and CDS spectrometers on September 21, 1996.

---------------------------------------------------------
Title: A chromospheric response to pulse beam heating (abstract)
Authors: Heinzel, P.
1998PAICz..88..137H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Flare Multi-Line 2D-SPECTROSCOPY
Authors: Mein, P.; Mein, N.; Malherbe, J. -M.; Heinzel, P.; Kneer,
   F.; von Uexkull, M.; Staiger, J.
1997SoPh..172..161M    Altcode: 1997ESPM....8..161M
  A small flare was observed at the Teide Observatory on October 5,
  1994. Simultaneous data were obtained at the German Vacuum Tower
  Telescope (VTT) with the MSDP spectrograph providing high-resolution
  imaging spectroscopy in two chromospheric lines, and the Gregory Coudé
  Telescope (GCT) providing information about the magnetic field. Basic
  flare characteristics are:

---------------------------------------------------------
Title: Formation of CA II Lines in Solar Prominences
Authors: Gouttebroze, P.; Vial, J. -C.; Heinzel, P.
1997SoPh..172..125G    Altcode: 1997ESPM....8..125G
  We compute the profiles of the resonance lines and infrared
  triplet of ionized calcium emitted by some representative models of
  prominences. These models consist of plane-parallel slabs of different
  temperatures, pressures and thicknesses, standing vertically above
  the solar surface. These slabs are assumed to be observed at the limb,
  and to be perpendicular to the line of sight. They are irradiated by
  the Sun on both sides, and the incoming intensities, at every relevant
  wavelength, are taken from observations. The model atom includes 3
  stages of ionization (Cai, Caii and Caiii) with 5 discrete levels for
  Caii. We study the relations between emitted intensities and physical
  properties of the slabs, and compare the intensities emitted in Caii and
  hydrogen lines for the same set of models. As a result of ionization,
  the intensity decreases more rapidly with temperature in Caii lines than
  in Hi lines, so that the ratio of Caii to Hi line intensities may be
  used as a temperature indicator. The intensity ratio between resonance
  and infrared lines of Caii depends principally on the optical thickness
  of the structure. At high pressure and low temperature, the ratio
  Caii 8542Å/Hβ is found to increase with pressure. This behaviour,
  which is due to the saturation of Hβ, is opposite to that found by
  Heasley and Milkey (1978) for low pressures (optically thin structures).

---------------------------------------------------------
Title: Optical and Radio Spectral Analysis of a Recurrent Surge
Authors: Kotrč, Pavel; Schmieder, Brigitte; Karlický, Marian;
   Heinzel, Petr
1997SoPh..172..199K    Altcode: 1997ESPM....8..199K
  Coordinated observations obtained at Meudon (MSDP) and at Ondřejov
  provide surge spectra in optical range (Hα, Hβ, Hγ, Hµ, Ca H and
  K lines) and in radio range. The MSDP data allowed us to follow the
  time evolution of the surge. The spectra of Balmer lines were used to
  derive the electron density of the expelled cool material. The radio
  bursts indicate that the acceleration of electrons took place in the
  low and dense atmosphere, giving a good argument for a reconnection
  near the transition region.

---------------------------------------------------------
Title: Solar and heliospheric plasma physics. Proceedings. 8th
    European Solar Physics Meeting, Halkidiki (Greece), 13 - 18 May 1996.
Authors: Heinzel, P.; Simnett, G.
1997SoPh..172....1H    Altcode: 1997ESPM....8....1H
  The main topic was the interaction of the Sun with the heliosphere,
  focused on first results from SOHO and new results from Ulysses. The
  following topics were dealt with: solar dynamos, solar shape, convection
  zone, solar pulsations, solar activity, solar atmosphere, solar corona,
  solar spectra, solar prominences, solar flares, UV spectra, solar wind,
  radiowave emissions, solar instruments.

---------------------------------------------------------
Title: NLTE Analysis of SUMER Filament Observations on SOHO
Authors: Heinzel, P.; Schmieder, B.; Vial, J. -C.
1997ESASP.404..427H    Altcode: 1997cswn.conf..427H
  No abstract at ADS

---------------------------------------------------------
Title: A Comparison of Two Approximations for the Cooling of Hot
    Post-Flare Loops
Authors: Varady, M.; Heinzel, P.
1997ESASP.404..705V    Altcode: 1997cswn.conf..705V
  No abstract at ADS

---------------------------------------------------------
Title: Dynamics and evolution of the post-flare loops of June 1992
Authors: Wiik, J. E.; van Driel-Gesztely, L.; Schmieder, B.;
   Heinzel, P.
1997AdSpR..20.2345W    Altcode:
  Observations in X-rays (Yohkoh/SXT) and in Hα of a system of post-flare
  loops which developed after a flare on 25 June 1992 provide a unique
  set of data for a study of the relationship between the hot and cool
  post-flare loops as they evolve. Through a study of the magnetic
  configuration in which the flare occurred, we are able to reconstruct
  the true, 3D geometry of the loops. We derive the bulk-flow velocities
  along the loop as a function of height using Doppler velocities and
  the results from the loop reconstruction. We also provide a set of
  relative altitude data. These results are used to check the validity
  of the reconnection model in the frame of the cooling time needed to
  cool X-ray loops to Hα temperature.

---------------------------------------------------------
Title: Structure and Dynamics of Post-Flare Loops
Authors: Varady, M.; Heinzel, P.
1997HvaOB..21...33V    Altcode:
  We briefly review basic properties of the post-flare loops and their
  structural and dynamical characteristics. Several new results have been
  recently published using the Yohkoh SXT images, simultaneously obtained
  with high-resolution H-alpha data. We pay a particular attention to
  the problem of cooling times of hot loops.

---------------------------------------------------------
Title: Post-Flare Loops of 26 June 1992, III
Authors: Wiik, J. E.; Schmieder, B.; Heinzel, P.; Roudier, T.
1996SoPh..166...89W    Altcode:
  Post-flare loops were observed on June 26, 1992 in the Hα line
  with the Multichannel Subtractive Double-Pass spectrograph (MSDP)
  on Pic-du-Midi and with the Swedish telescope on La Palma. The highly
  dynamic loops are inhomogeneous (blobs). The cool loops were observed
  10-12 hours after the X 3.9 class flare which had a maximum on June
  25 at 20∶11 UT. From 2D images obtained with the MSDP on June 26 we
  derive Hα intensities and Doppler velocities of the loop plasma. Using
  a geometrical reconstruction technique we show that these loops are
  mainly perpendicular to the solar surface and have the shape of a
  dipole magnetic configuration. We derive the bulk-flow velocities along
  the loop as a function of height using the Doppler velocities and the
  results from the loop reconstruction. Where the Doppler velocities are
  too small, we derive the bulk-flow velocities from the displacements
  of the falling blobs. We discuss existing deviations from free-fall
  velocity in the lower parts of the loops.

---------------------------------------------------------
Title: Post-Flare Loops of 26 June 1992, II
Authors: Schmieder, B.; Heinzel, P.; Van Driel-Gesztelyi, L.; Lemen,
   J. R.
1996SoPh..165..303S    Altcode:
  We observed the large post-flare loop system, which developed after the
  X 3.9 flare of 25 June 1992 at 20∶11 UT, in Hα with the Multichannel
  Subtractive Double Pass Spectrograph at Pic-du-Midi and in X-rays with
  the it Yohkoh/SXT instrument. Following the long-term development of
  cool and hot plasmas, we have determined the emission measure of the
  cool plasma and, for the first time, the temporal evolution of the
  hot-loop emission measure and temperature during the entire gradual
  phase. Thus, it was possible to infer the temporal variation of electron
  densities, leading to estimates of cooling times. A gradual decrease of
  the hot-loop emission measure was observed, from 4 × 10<SUP>30</SUP>
  cm<SUP>−5</SUP> at 23∶00 UT on 25 June 1992 to 3 × 10<SUP>28</SUP>
  cm<SUP>−5</SUP> at 13∶10 UT on 26 June 1992. During the same period,
  the temperature decreased only slowly from 7.2 to 6.0 × 10<SUP>6</SUP>
  K. Using recent results of NLTE modeling of prominence-like plasmas,
  we also derive the emission measure of cool Hα loops and discuss
  their temperature and ionisation degree. During two hours of Hα
  observations (11-13 hours after the flare) the averaged emission
  measure does not show any significant change, though the amount
  of visible cool material decreases and the volume of the loops
  increases. The emission measure in Hα, after correction for the
  Doppler-brightening effect, is slightly lower than in soft X-rays. Since
  the hot plasma seems to be more spatially extended, we arrive at
  electron densities in the range n<SUB>infe</SUB><SUP>supho</SUP>≤
  n<SUB>infe</SUB><SUP>supcool</SUP>∼ 2 × 10<SUP>10</SUP>
  cm<SUP>−3</SUP> at the time of the Hα observations.

---------------------------------------------------------
Title: Cloud model with variable source function for solar Hα
    structures.
Authors: Mein, N.; Mein, P.; Heinzel, P.; Vial, J. -C.; Malherbe,
   J. M.; Staiger, J.
1996A&A...309..275M    Altcode:
  The "cloud model" used to derive the physical parameters of solar
  chromospheric features is extended to the cases of non-constant
  source function and of velocity gradients. This model assumes a given
  relationship between the source function and the opacity of the cloud
  which is derived from non-LTE modelling. An algorithm using 4 points
  of the H<SUB>alpha</SUB>_ profile is proposed to derive the optical
  thickness, the line-of-sight velocity and the dopplerwidth. The
  results are compared with a 5-points inversion which does not use the
  given relationship between source function and opacity. Effects of the
  uncertainty about the radiation coming from the underlying chromosphere,
  as well as effects of data noise, are discussed. The inversion method
  is illustrated by some examples of observed profiles obtained with
  the MSDP spectrograph of the VTT telescope (Teide Observatory).

---------------------------------------------------------
Title: A Complex Diagnostic of Solar Prominences
Authors: Heinzel, P.; Bommier, V.; Vial, J. C.
1996SoPh..164..211H    Altcode:
  We use the polarimetric and intensity measurements of Hα and HeI
  D<SUB>3</SUB> lines in solar prominences to derive the true geometrical
  thickness for several quiescent prominences. The electron densities,
  derived from the collisional depolarization in Hα by Bommier et
  al. (1994), are used to evaluate the thickness from the emission
  measure. The emission measure was obtained from the theoretical
  correlation with the Hα integrated intensity, according to Gouttebroze,
  Heinzel, and Vial (1993). Theoretical electron densities obtained by
  latter authors are also compared with those of Bommier et al. (1994) and
  we find a very good agreement between them. The prominence geometrical
  thickness exhibits a relatively large range of values from about 100 km
  up to a few 10<SUP>4</SUP> km. The plasma densities vary by almost two
  orders of magnitude in the observed structures, but the total column
  mass in the direction perpendicular to the prominence sheet seems to
  be fairly constant for the set of prominences studied.

---------------------------------------------------------
Title: Structure and evolution of post-flare loops: analysis of
    YOHKOH and MSDP observations
Authors: Schmieder, B.; Heinzel, P.; Wiik, J. E.; Lemen, J.; Hiei, E.
1996AdSpR..17d.111S    Altcode: 1996AdSpR..17..111S
  Using coordinated observations of the June 26 1992 post-flare loops
  (Yohkoh-SXT and MSDP at Pic-du-Midi), we have analyzed the physical
  conditions in both hot and cool loops and studied their spatial
  structure and temporal evolution. Coalignment of high-resolution images
  from SXT and MSDP indicates that the cool Hα loops are located just
  below the hot ones and that the whole loop system grows in time with
  a velocity 1.4 km s^-1. The temperature of hot loops as derived from
  SXT data amounts to 5 x 10^6 K, while the cool loops have temperatures
  around 10^4 K. The electron density of hot loops was estimated from
  SXT emission-measure analysis to 7 x 10^9 cm^-3, while Hα integrated
  intensity gives an electron density in cool loops of 2.2 x 10^10
  cm^-3. With these plasma parameters we have solved the energy equation
  in order to estimate the cooling time. The basic result of this work
  is that the cooling time is comparable to the characteristic growing
  time of the loop system (~ 1500 - 2000 sec), which is in agreement
  with the scenario of the post-flare loop system development.

---------------------------------------------------------
Title: NLTE modelling based on SOHO/SUMER and GBO coordinated
    observations.
Authors: Heinzel, P.
1996joso.proc...92H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Observations and Analysis of Surges in Chromosphere and
    Lower Corona
Authors: Kotrc, P.; Schmieder, B.; Karlický, M.; Heinzel, P.
1996RoAJ....6...69K    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Hot and Cool Post-Flare Loops: Formation and Dynamics
Authors: Schmieder, B.; Heinzel, P.; van Driel-Gesztelyi, L.; Wiik,
   J. E.; Lemen, J.
1996mpsa.conf..211S    Altcode: 1996IAUCo.153..211S
  No abstract at ADS

---------------------------------------------------------
Title: Dynamics of solar magnetic arches in the photosphere and
    the chromosphere.
Authors: Mein, P.; Demoulin, P.; Mein, N.; Engvold, O.; Molowny-Horas,
   R.; Heinzel, P.; Gontikakis, C.
1996A&A...305..343M    Altcode:
  Mass motions in chromospheric arch filaments have been observed
  with imaging spectroscopy (MSDP) at the VTT telescope of the Teide
  Observatory. Coordinated observations of time sequences of continuum
  images were carried out at the SVST telescope of the Observatorio
  del Roque de los Muchachos, which provided transverse velocities of
  photospheric tracers, by "local correlation tracking." Hα profiles
  along 3 arch filaments are analysed in terms of "differential
  cloud MODel", to discuss the Doppler velocities of chromospheric
  material. Models of ascending arches with downflows in both legs
  are investigated. The gas pressure is neglected, but the free-fall
  equations are integrated versus time (non-stationary case). We first
  assume circular lines of force with constant radius. We can account
  for chromospheric velocities, but we cannot fit the slow motion of
  footpoints derived from photospheric tracers. A better agreement is
  obtained by assuming lines of force with fixed footpoints and variable
  radius. Typical values are: half distance between footpoints of 10 to
  15Mm, upward velocity at the top of loops of 4km/s after an integration
  time of 800s. The obtained values are consistent with the sizes and
  the lifetime of arch filaments.

---------------------------------------------------------
Title: Relative Altitude of Hot and Cool Post-Flare Loops
Authors: van Driel-Gesztelyi, L.; Schmieder, B.; Wiik, J. E.; Tarbell,
   T.; Heinzel, P.; Kitai, R.; Funakoshi, Y.; Anwar, B.
1996ASPC..111..359V    Altcode: 1997ASPC..111..359V
  The authors collected a unique set of data obtained simultaneously at
  4 different ground based observatories and with the Yohkoh satellite
  to study the relationship between hot X-ray and cool Hα post-flare
  loops as they evolved during the long gradual phase of the X3.9 flare
  which occurred on 25 June 1992. They found reasonably good agreement
  between the computed 'theoretical' cooling times and the 'observed'
  cooling times derived from the relative altitudes of hot and cool
  loops. Taking into account evolutionary effects, the authors also found
  similar shape and configuration of hot and cool loops during the entire
  observing period and confirmed that at any time hot loops are at higher
  altitude than cool loops, suggesting that cool loops indeed descend
  from hot loops. The results provide support for the reconnection model.

---------------------------------------------------------
Title: High resolution flare observations with multi-line imaging
    spectroscopy.
Authors: Mein, P.; Heinzel, P.; Malherbe, J. -M.; Staiger, J.
1996joso.proc...68M    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: On the nature of bright rims of filaments
Authors: Heinzel, Petr; Kotrč, Pavel; Mouradian, Zadig; Buyukliev,
   Georgi T.
1995SoPh..160...19H    Altcode:
  A filament with a very bright rim was observed in the Hα line on May
  11, 1989, using the Meudon spectroheliograph. Absolute calibration of
  the spectroheliogram allows us to express the intensities in particular
  sites of the filament, in its bright rim and inside the surrounding
  chromosphere. From a large number of photometric scans, we obtained a
  histogram of the intensity excess of the bright rim relative to the
  quiet chromosphere. The mean value of this excess amounts to about
  4%. We present a theoretical explanation of bright rims, based on
  the nature of Hα radiative diffusion in the filaments. Computed NLTE
  model of the filament leads to a rim intensity excess which is in good
  agreement with our observations.

---------------------------------------------------------
Title: Multilevel NLTE radiative transfer in isolated atmospheric
structures: implementation of the MALI-technique.
Authors: Heinzel, P.
1995A&A...299..563H    Altcode:
  We have developed and extensively tested a new multilevel NLTE transfer
  code for isolated solar atmospheric structures (loops, prominences,
  spicules etc.). The code is based on the MALI approach of Rybicki &amp;
  Hummer (1991, 1992) to multilevel accelerated lambda iterations. It is
  demonstrated that this method is fully capable of treating a difficult
  problem of NLTE hydrogen excitation and ionization equilibrium, provided
  that we linearize the preconditioned statistical equilibrium equations
  with respect to atomic level populations and the electron density. With
  this generalization of the original MALI approach, the numerical code
  is robust and stable. As compared to the standard linearization method
  of Auer &amp; Mihalas (1969), the new MALI code designed for 1D slabs
  is more than one order of magnitude faster and its accuracy is quite
  satisfactory. We discuss several details of our implementation of the
  MALI technique to isolated, externally irradiated, 1D structures and
  finally draw some future prospects.

---------------------------------------------------------
Title: Relation between Cool and Hot Post-Flare Loops of 26 June
    1992 Derived from Optical and X-Ray (SXT-YOHKOH) Observations
Authors: Schmieder, B.; Heinzel, P.; Wiik, J. E.; Lemen, J.; Anwar,
   B.; Kotrc, P.; Hiei, E.
1995SoPh..156..337S    Altcode:
  We have analyzed the physical conditions of the plasma in post-flare
  loops with special emphasis on dynamics and energy transport using
  SXT-data (hot plasma) and optical ground-based data from Pic du Midi,
  Wrocław, and Ondřejov (cool plasma). By combining the Hα observations
  with the SXT images we can understand the relationship between cool and
  hot plasmas, the process of cooling post-flare loops and the mechanism
  which maintains the long duration of these loops. Using recent results
  of NLTE modeling of prominence-like plasmas, we derive the emission
  measure of cool Hα loops and this gives us a realistic estimate of
  the electron density (2.2 × 10<SUP>10</SUP> cm<SUP>−3</SUP>). Then,
  by comparing this emission measure with that of hot loops derived from
  SXT data, we are able to estimate the ratio between electron densities
  in hot and cool loops taking into account the effect of geometrical
  filling factors. This leads to the electron density in hot loops 7 ×
  10<SUP>9</SUP> cm<SUP>−3</SUP>. We also derive the temperature of
  hot X-ray loops (≃ 5.5 × 10<SUP>6</SUP> K), which, together with
  the electron density, provides the initial values for solving the
  time-dependent energy balance equation. We obtain the cooling times
  which are compared to a typical growth-time of the whole loop system
  (∼ 2000 s). In the legs of cool Hα loops, we observe an excess
  of the emission measure which we attribute to the effect of Doppler
  brightening (due to large downflow velocities).

---------------------------------------------------------
Title: Dynamic loops in the corona
Authors: Heinzel, P.
1994ESASP.373..133H    Altcode: 1994soho....3..133H
  No abstract at ADS

---------------------------------------------------------
Title: Theoretical correlations between prominence plasma parameters
    and the emitted radiation.
Authors: Heinzel, P.; Gouttebroze, P.; Vial, J. -C.
1994A&A...292..656H    Altcode:
  Recently a set of 140 prominence NLTE models has been computed using
  the best available numerical techniques (Gouttebroze et al. 1993,
  hereafter GHV). Models are represented by one-dimensional (1D) slabs
  vertically standing on the solar surface and irradiated by photospheric
  and chromospheric radiation. They are parametrized by the gas pressure
  and temperature (uniform), the geometrical thickness of the 1D slab,
  the microturbulent velocity and the height above the solar surface. As
  outputs we obtained several physical quantities and optical parameters
  like the electron density, the total hydrogen density, the optical
  thickness in hydrogen lines and continua, spectral line intensities
  etc. (see GHV). In order to establish mutual correlations between
  various plasma parameters and the basic characteristics of the
  synthesized hydrogen spectrum, we construct some basic correlation
  curves. A very important relation already mentioned in GHV concerns the
  plasma emission measure found to be closely related to the integrated
  intensity of the Balmer Hα line. We present several other correlations
  which can be divided into four categories: (i) relations between
  radiation properties themselves; (ii) radiation properties versus
  plasma parameters; (iii) the Hα source function behaviour; and (iv)
  correlations between plasma parameters. Together with the 24 presented
  figures, we discuss the physical interpretation of these correlations
  and we give some hints for their application to the observed data. When
  appropriate, we also compare our results with existing observations.

---------------------------------------------------------
Title: Dynamics of post-flare loops observed on June 26, 1992
Authors: Wiik, J. E.; Schmieder, B.; Heinzel, P.; Roudier, T.
1994ESASP.373..207W    Altcode: 1994soho....3..207W
  No abstract at ADS

---------------------------------------------------------
Title: Chromospheric and transition-region heating phenomena:
    coordinated GBO and SOHO observations
Authors: Heinzel, P.; Kotrc, P.; Karlicky, M.; Nejezchleba, T.;
   Knizek, M.
1994ESASP.373..369H    Altcode: 1994soho....3..369H
  No abstract at ADS

---------------------------------------------------------
Title: Coordinated optical and YOHKOH observations of 26 June 1992
    flare loops
Authors: Heinzel, P.; Kotrč, P.; Schmieder, B.; Hiei, E.; Anwar, B.
1994SSRv...70..181H    Altcode:
  Optical spectra of large flare loops were detected by the Ondřejov
  Multichannel Flare Spectrograph (MFS) during coordinated observations
  with MSDP at Pic du Midi (Hα) and the soft X-ray telescope (SXT)
  on Yohkoh. The CCD video images taken by the MFS slit-jaw camera
  document the time-development of the flare loops as seen through the
  Hα filter. Preliminary analysis of the MSDP images shows the intensity
  structure of the cool flare loops and their velocity fields. From the
  spectra we can clearly see the intensity variations along the cool
  loops. SXT images show the structure of hot X-ray loops similar to
  that of cool loops. Special attention is devoted to the bright tops,
  simultaneously observed in X-rays, Hα and other optical lines. Based
  on a preliminary analysis of the optical spectra, we speculate about
  possible mechanisms leading to an observed bright emission at the tops
  of cool loops. We suggest that direct soft X-ray irradiation of cool
  loops at their tops could be, at least partly, responsible for such
  a strong brightening.

---------------------------------------------------------
Title: Energy Transport and Dynamics
Authors: Schmieder, B.; Peres, G.; Enome, S.; Falciani, R.; Heinzel,
   P.; Hénoux, J. C.; Mariska, J.; Reale, F.; Rilee, M. L.; Rompolt, B.;
   Shibasaki, K.; Stepanov, A. V.; Wülser, J. P.; Zarro, D.; Zharkova, V.
1994SoPh..153...55S    Altcode:
  We report findings concerning energy transport and dynamics in flares
  during the impulsive and gradual phases based on new ground-based and
  space observations (notably fromYohkoh). A preheating sometimes occurs
  during the impulsive phase. CaXIX line shifts are confirmed to be
  good tracers of bulk plasma motions, although strong blue shifts are
  not as frequent as previously claimed. They often appear correlated
  with hard X-rays but, forsome events, the concept that electron beams
  provide the whole energy input to the thermal component seems not
  to apply. Theory now yields: new diagnostics of low-energy proton
  and electron beams; accurate hydrodynamical modeling of pulse beam
  heating of the atmosphere; possible diagnostics of microflares (based
  on X-ray line ratio or on loop variability); and simulated images of
  chromospheric evaporation fronts. For the gradual phase, the continual
  reorganization of magnetic field lines over active regions determines
  where and when magnetic reconnection, the mechanism favoured for energy
  release, will occur. Spatial and temporal fragmentation of the energy
  release, observed at different wavelengths, is considered to be a
  factor as well in energy transport and plasma dynamics.

---------------------------------------------------------
Title: On the Occurrence of Blue Asymmetry in Chromospheric Flare
    Spectra
Authors: Heinzel, Petr; Karlicky, Marian; Kotrc, Pavel; Svestka, Zdenek
1994SoPh..152..393H    Altcode:
  We present observations of optical spectra of a flare in which blue line
  asymmetry was seen for more than 4 min close to the flare onset. The
  maximum blue asymmetry coincided with the maximum of a hard X-ray
  and microwave burst. We discuss possible interpretations of the blue
  asymmetry and conclude that the most plausible one is electron-beam
  heating with return current. Although this process predicts downflows
  in the lower transition region and upper chromosphere, its ultimate
  effect on the line profiles can be blue asymmetry: the upper layers
  moving away from us absorb the radiation of the red peak thus lowering
  its intensity in comparison to the blue one.

---------------------------------------------------------
Title: Chromospheric fine structure: Black &amp; white mottles
Authors: Heinzel, P.; Schmieder, B.
1994A&A...282..939H    Altcode:
  H-alpha observations of the chromosphere have been obtained
  on June 17, 1986 with a high spatial resolution using the MSDP
  (Multichannel Subtractive Double Pass) spectrograph operating
  at Pic du Midi observatory. Various fine structures are observed
  in the chromosphere: bushes of fibrils around supergranules and
  fibrils (mottles) in the rosettes. They are relatively stable, but
  line-of-sight velocities +/- 5-10 km/s are observed at the boundaries
  of supergranules (rosettes). Velocity images exhibit finer structures
  than intensity ones, with no cospatial relationship between both of
  them. Typical H-alpha line profiles of dark and bright (black &amp;
  white) mottles, constructed from 11 MSDP channels, are used to derive
  the physical conditions in these structures. Non-local thermodynamic
  equilibrium (NLTE) models of dark and bright mottles are represented
  by a grid of prominence-like models of Goutebroze et al. (1993). It is
  demonstrated that higher-pressure models(p<SUB>g</SUB> approximately =
  0.5-1 dyn/sq cm) with temperature around 10<SUP>4</SUP> K naturally
  explain the profiles of both dark and bright structures. By introducing
  a generalized two-cloud model with non-uniform source function, we
  account schematically for a shear-type velocity field. However, the
  velocities are found to be of a secondary importance when the broad
  U-shaped profiles formation is considered. We conclude that dark
  and bright mottles have a similar nature and that their brightness
  difference is predominantly due to pressure variations of the plasma
  injected into the rosette flux tubes. Finally, we discuss the ambiguity
  of H-alpha contrast profiles and comment on applicability of the
  classical cloud model.

---------------------------------------------------------
Title: Fine structures of the solar chromosphere
Authors: Schmieder, B.; Heinzel, P.; Tsiropoula, G.; Alessandrakis,
   C. E.
1994ASIC..433..151S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Spectral Analysis of a Quiescent Filament
Authors: Kotrc, P.; Heinzel, P.; Gorshkov, A. V.; Kononovich, E. V.;
   Kupryakov, Yu. A.; Smirnova, O. B.
1994scs..conf..361K    Altcode: 1994IAUCo.144..361K
  The authors have determined principal plasma parameters in a filament
  by applying the appropriate cloud model to several observed spectral
  lines. Then they compared them to prominence models from the recent
  numerical NLTE modelling of Gouttebroze et al. (1993). Some preliminary
  results of such an attempt are described and related problems are
  briefly discussed.

---------------------------------------------------------
Title: Theoretical Correlations Between Various Prominence Parameters
Authors: Heinzel, P.; Gouttebroze, P.; Vial, J. -C.
1994scs..conf..439H    Altcode: 1994IAUCo.144..439H
  The authors present some examples of important correlations between the
  prominence plasma parameters and radiation properties. For example,
  the plasma emission measure was found to be closely related to the
  integrated Hα line intensity which provides a new diagnostic tool
  for determination of plasma densities.

---------------------------------------------------------
Title: Evolution of an Eruptive Prominence and its Magnetic System
    on 2 September 1991
Authors: Rudawy, P.; Rompolt, B.; Kotrič, P.; Heinzel, P.; Knižek,
   M.; Garczyńska, I.; Cader-Sroka, B.
1994emsp.conf...95R    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Contrast of Filament Bright Rims
Authors: Kononovich, E. V.; Smirnova, O. B.; Heinzel, P.; Kotrc, P.
1994scs..conf..365K    Altcode: 1994IAUCo.144..365K
  Hα filtergrams were measured in order to specify the bright rims
  contrast at different points along the line profile. The mean
  contrast value in the line center is about 25 percent. The bright
  rims interpretation as the bases of magnetic structures supporting
  the filaments is suggested.

---------------------------------------------------------
Title: Dragging out of the near-surface magnetic fields during the
    prominence eruptions
Authors: Rudawy, P.; Rompolt, B.; Kotrč, P.; Heinzel, P.; Knižek, M.
1994smf..conf..372R    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Solar coronal structures
Authors: Rusin, Vojtech; Heinzel, Petr; Vial, Jean-Claude
1994scs..conf.....R    Altcode: 1994IAUCo.144.....R
  No abstract at ADS

---------------------------------------------------------
Title: Electron Densities in Solar Prominences
Authors: Wiik, J. E.; Heinzel, P.; Schmieder, B.
1994scs..conf..381W    Altcode: 1994IAUCo.144..381W
  The authors concentrate on the determination of electron densities,
  using the MSDP spectrograph at Pic du Midi. They discuss a new approach
  for diagnosing the electron densities by comparing the observed Hα
  intensities with theoretically predicted variations of the line-center
  intensity versus N<SUB>e</SUB>.

---------------------------------------------------------
Title: Black and White Mottles
Authors: Heinzel, P.; Schmieder, B.
1994emsp.conf...81H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: The hydrogen spectrum of model prominences.
Authors: Gouttebroze, P.; Heinzel, P.; Vial, J. C.
1993A&AS...99..513G    Altcode:
  The emission of hydrogen lines and continua from solar prominences is
  investigated using a set of 140 simple models, covering the range of
  physical conditions usually assumed for these objects. These models
  are plane-parallel, isobaric and isothermal. The computations have been
  carried out using a 20 level plus continuum hydrogen atom, and taking
  into account the effects of partial frequency redistribution in the
  Lyman-alpha and beta lines. The aim of these computations is twofold:
  firstly, to describe the variations of hydrogen lines and continua
  emitted by prominences when physical conditions vary. Secondly, to
  provide observers with some diagnostic tool to interpret data such as
  intensity ratios, line widths, etc... The results of computations are
  given as mixed table-figure panels, each of them corresponding to a
  given model and summarizing the associated physical parameters and
  the principal features of the emitted hydrogen spectrum. Finally,
  for some specific parameters (or couple of parameters), we present
  figures illustrating the variations of these quantities across the
  whole set of models.

---------------------------------------------------------
Title: Book Review: Solar interior and atmosphere / U Arizona
    Press, 1991
Authors: Heinzel, P.; Priest, E. R.; Heinzel, P.
1993SoPh..144..203H    Altcode: 1993SoPh..144..203C
  No abstract at ADS

---------------------------------------------------------
Title: Book Review: Applying Fractals in Astronomy
Authors: Martens, P. C.; Kleczek, Josip; Heinzel, P.
1993SoPh..143..401M    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Book Review: Eruptive solar flares / Springer-Verlag, 1992
Authors: Heinzel, P.
1993SoPh..143..402H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Pulse-beam heating in flare loops.
Authors: Heinzel, Petr; Karlicky, M.
1992ESASP.348..237H    Altcode: 1992cscl.work..237H
  Using a 1D hydbrid code, the authors evaluate a response of the flare
  loop atmosphere to a series of very short electron beam pulses with
  subsecond duration. Loop dynamics and energy balance are treated by
  solving the standard set of hydrodynamic equations, while the beam
  deceleration in denser atmospheric layers is evaluated by using a
  particle simulation technique. Ionization of hydrogen below T ≍
  10<SUP>4</SUP>K is obtained by solving simultaneously the time-dependent
  non-LTE problem for a three-level hydrogen atom with continuum. The
  resulting electron densities are then used to compute radiation losses
  at each time step. The authors discuss the behaviour of time-dependent
  heating, the ionization structure of the chromosphere, and the role of
  relaxation processes. A series of short-duration electron beam pulses
  represents schematically the non-stationary heating in the flare
  loops. However, the time-dependent radiation-hydrodynamical approach
  used in this paper can also be applied to study other processes taking
  place in coronal loops.

---------------------------------------------------------
Title: Book Review: Exploring the sun; solar science since Galileo /
    Johns Hopkins, 1991
Authors: Heinzel, P.
1992SoPh..141..411H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Book reviews
Authors: Trams, N. R.; Heinzel, P.
1992SoPh..141..411T    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Determination of plasma parameters in a quiescent prominence
Authors: Wiik, J. E.; Heinzel, P.; Schmieder, B.
1992A&A...260..419W    Altcode:
  We present H-alpha observations and analysis of a quiescent, polar crown
  prominence observed on June 11, 1988 with the MSDP spectrograph at the
  Pic du Midi Observatory. Two-dimensional maps of H-alpha intensities and
  line-of-sight velocities have been obtained. The large-scale velocity
  pattern consisting of cells and elongated structures is stable on
  a time scale of about 1 min, but evolves continuously and undergoes
  large changes in shape and amplitude during one hour. This behavior
  of the velocity field suggests the presence of twists in flux ropes
  or shear motions. Further, comparing the absolute observed intensities
  with values from non-LTE radiative computations we estimate the range
  of electron densities, source functions and optical thicknesses in
  different parts of the prominence. For upper parts of the prominence
  we obtain electron densities in the range 1 - 5 x l0 exp 10/cu cm.

---------------------------------------------------------
Title: The fine structure of prominences.
Authors: Heinzel, P.; Vial, J. -C.
1992ESASP.344...57H    Altcode: 1992spai.rept...57H
  Ground-based observations evidence in prominences a fine structure both
  in density and velocity fields at a subarcsec scale. The modeling of
  such structures is necessary in order to account for heating and cooling
  processes which depend critically on the geometry and the structure of
  the magnetic field. For a rigorous treatment of the radiative losses,
  one needs to solve the full NLTE problem especially in UV lines,
  which are critical for the energy balance. Although some attempts
  have already been made to model individual fine-structure elements,
  quiescent prominences are still mostly considered as one-dimensional
  structures. We discuss current improvements such as two-dimensional
  geometry and bundle of threads.

---------------------------------------------------------
Title: Structure and Dynamics of Cool Flare Loops
Authors: Heinzel, P.; Schmieder, B.; Mein, P.
1992SoPh..139...81H    Altcode:
  MSDP observations of the 16 May, 1981 two-ribbon flare are used to
  study the physical structure and the dynamical behaviour of cool flare
  loops. The loops have been detected in the Hα line just after the
  flare maximum and they appeared in absorption against the disk. Using
  the first-order differential cloud model (DCM1) technique, we derive
  empirically some basic plasma parameters at 15 points along one loop
  leg. The flow velocities and the true heights have been reconstructed
  with respect to a geometrical projection. Subsequently, detailed
  non-LTE models of cool loops have been constructed in order to fit Hα
  source function values previously derived from DCM1 analysis. It is
  demonstrated that this source function is rather sensitive to the radial
  component of the flow velocity (the so-called Doppler brightening)
  and to enhanced irradiation of the loops from the underlying flare
  ribbons. In this way, we have been able to estimate quantitatively
  all plasma parameters which determine the physical structure of cool
  loops (i.e., the temperature, pressure, density), as well as the
  momentum-balance condition within the loops. For these dark loops we
  have arrived at relatively low gas pressures of the order of 0.1-0.5
  dyne cm<SUP>-2</SUP> with corresponding electron densities around
  10<SUP>11</SUP> cm<SUP>-3</SUP>. Pressure-gradient forces have been
  found to be of small importance in the momentum-balance equation, and
  thus they cannot explain departures from a free-fall motion found in our
  MSDP data analysis. We propose three possible solutions to this problem.

---------------------------------------------------------
Title: Hydrogen Photoionization Rates for Chromospheric and Prominence
    Plasmas
Authors: Rudawy, P.; Heinzel, P.
1992SoPh..138..123R    Altcode:
  New values of hydrogen photoionization rates for subordinate continua
  arising from bound levels with the principal quantum number i = 2-5
  have been evaluated numerically, using an extensive compilation of the
  observed photospheric radiation fields. These rates can be directly
  incorporated into the equations of statistical equilibrium as so-called
  fixed rates. We tabulate the photoionization rates and equivalent
  radiation temperatures for various heights above the photosphere,
  which is particularly useful for chromospheric and prominence non-LTE
  modeling. Finally, we compare our results with those previously obtained
  by other authors.

---------------------------------------------------------
Title: Subsecond Variations of HXR and Hα Flare Emission
Authors: Heinzel, P.; Karlicky, M.
1992LNP...399..359H    Altcode: 1992esf..coll..359H; 1992IAUCo.133..359H
  For a series of electron beam pulses, we have computed the
  time-dependent chromospheric heating and the corresponding hard X-ray
  (HXR) flux. Moreover, by solving the time-dependent NLTE problem for
  hydrogen, we theoretically predict the Ha-line intensity variations
  on sub-second time scales. Both HXR-fluxes and Ha wing intensities
  do exhibit a spiky behaviour, consistent with short pulse-beam
  heating. However, the spikes in Ha are unexpectedly inverse, i.e. the
  line intensity decreases during the beam heating. They correlate rather
  well with HXR emission peaks computed for 24 keV channel. We compare our
  theoretical results with recent observations of Kiplinger et al. (1991).

---------------------------------------------------------
Title: Fine structure analysis of a prominence in H-alpha and
    coronal lines
Authors: Wiik, J. E.; Schmieder, B.; Noens, J. C.; Heinzel, P.
1992sws..coll..131W    Altcode:
  Prominence observations made simultaneously with the MSDP spectrograph
  and with the coronagraph at Pic du Midi are presented. The existence
  of a coronal cavity is discussed. 2D maps of H-alpha intensities
  and the line-of-sight velocities have been obtained. The behavior
  of the velocity field suggests the presence of twists along flux
  ropes or shear motions. Further, using a probabilistic approach to
  the H-alpha-line formation, we estimate the range of temperatures,
  electron densities and optical thicknesses in different parts of the
  prominence by fitting the observed H-alpha intensity profiles.

---------------------------------------------------------
Title: Plasma Parameters Derived from MSDP Observations of Cool
    Flare Loops
Authors: Heinzel, P.; Schmieder, B.; Mein, P.
1992LNP...399..134H    Altcode: 1992IAUCo.133..134H; 1992esf..coll..134H
  MSDP observations of 16 May 1981 two-ribbon flare are used to study the
  physical structure and dynamical behaviour of cool flare loops. The
  loops have been detected in the H line just after the flare maximum
  and they appeared in absorption against the disk. Using the first-order
  differential cloud model (DCM1) technique, we derive empirically some
  basic plasma parameters at 15 points along one loop leg. The flow
  velocities and true heights have been reconstructed with respect to
  a geometrical projection. Subsequently, detailed non-LTE models of
  cool loops have been constructed in order to fit H source-function
  values previously derived from DCM1 analysis. It is demonstrated that
  this source function is rather sensitive to the radial component
  of the flow velocity (the so-called Doppler brightening) and to
  the enhanced irradiation of the loops from the underlying flare
  ribbons. In this way, we have been able to estimate quantitatively
  all plasma parameters which determine the physical structure of
  cool loops (i. e. the temperature, pressure, density, etc.), as well
  as the momentum-balance condition within the loops. For these dark
  loops we have arrived at relatively low gas pressures of the order
  of 0.1 - 0.5 dyn cm-2 , with corresponding electron densities around
  1011 cm-3. Pressure-gradient forces have been found to be of small
  importance in the momentum-balance equation. However, the classical
  momentum equation is not capable of explaining significant departures
  from a free-fall motion under the gravity force, found from our MSDP
  data. We propose three possible explanations to this problem.

---------------------------------------------------------
Title: A Chromospheric Response to Pulse Beam Heating
Authors: Heinzel, Petr
1991SoPh..135...65H    Altcode:
  Starting from the new flare models of Karlický (1990) and Karlický
  and Hénoux (1991), we present here the first time-dependent numerical
  simulations of hydrogen plasma excitation and ionization on time scales
  of less than one second. These time scales are consistent with the spiky
  behaviour of the kinetic temperature produced by non-thermal collisional
  processes. Such temperature spikes represent a chromospheric response
  to a series of short-duration electron beam pulses which are supposed
  to heat the flare atmosphere. Self-consistent numerical solution
  of a simplified, time-dependent, non-LTE problem for a three-level
  hydrogen atom model with continuum allows us to predict theoretically
  a qualitative behaviour of the Hα line intensity variations on very
  short time intervals. Our Hα temporal profiles, evaluated at the line
  center and for Δλ = 1 Å, can be qualitatively compared with some
  recent flare observations obtained with high temporal resolution.

---------------------------------------------------------
Title: Chromospheric Inhomogeneities in Cool Stars - Possible Effect
    on Hydrogen Line Profiles
Authors: Heinzel, P.
1991ASIC..341..297H    Altcode: 1991sabc.conf..297H
  No abstract at ADS

---------------------------------------------------------
Title: Formation of hydrogen lines under the influence of turbulent
    electric fields in solar flares.
Authors: Heinzel, Petr
1990JQSRT..44..185H    Altcode:
  A new method of detecting low-frequency ion-sound turbulence in solar
  chromospheric flares is proposed. The method is based on analysis of the
  hydrogen Paschen γ line profiles, which exhibit - under the appropriate
  conditions - diagnostically important humps in the line wings around
  Δλ ≅ 1 Å. The author discusses the problem of Paschen γ line
  formation under the influence of low-frequency turbulent electric
  fields and compares his theoretical results with recent spectral
  observations. From comparison with the observed profile, the author
  derives a turbulent electric field mean intensity of F<SUB>0</SUB>
  ≅ 3 CGS.

---------------------------------------------------------
Title: Spectral line formation in plasmas under extreme or unusual
    conditions. Proceedings. Workshop on Spectral Line Formation in
    Plasmas Under Extreme or Unusual Conditions, Nice (France), 31 Aug -
    4 Sep 1987.
Authors: Peyraud, N.; Heinzel, P.; Hooper, C. F., Jr.
1990JQSRT..44.....P    Altcode:
  Contents: 1. Plasma electric fields. 2. Diagnostics of laboratory
  plasmas. 3. Spectral line formation and broadening. 4. Astrophysical
  plasmas.

---------------------------------------------------------
Title: On the Presence of High-frequency Turbulent Electric Fields
    in the August 7, 1960 Flare
Authors: Firstova, N. M.; Heinzel, P.; Kotrc, P.
1990BAICz..41...88F    Altcode:
  According to Oks (1978), the wings of some hydrogen Balmer lines
  observed in the spectrum of the moustache-like flare of August 7,
  1960 do exhibit theoretically predicted dips, which should indicate
  the presence of Langmuir turbulence. However, these features are rather
  subtle and thus several difficulties arise if one tries to identify them
  in the noisy spectra with typically many blends. Moreover, the Balmer
  profiles used for Oks' analysis were already 'filtered' in a special
  manner, which strongly affects the results. In view of these problems,
  consideration is given to whether these dips in this particular flare
  were real, starting with newly obtained microphotometric records. Using
  the same lines as Oks (i.e., H7, H8, H11-13), together with H14,
  none of the expected dips in the line wings were identified. All
  observational aspects of this analysis are discussed in detail, and
  new special observations are proposed. The role of electron density
  variations within the flare volume is also briefly discussed.

---------------------------------------------------------
Title: Hα diagnostics of 16 May 1981 flare loops.
Authors: Heinzel, P.; Mein, P.; Schmieder, B.
1990PDHO....7..272H    Altcode:
  MSDP observations (Meudon) of 16 May 1981 post-flare loops are used
  to derive the hydrogen plasma parameters in flare loops. The authors
  compare two recently developed methods: a differential cloud model
  and a probabilistic transfer technique.

---------------------------------------------------------
Title: Hydrogen Line Formation in Filamentary Prominences
Authors: Heinzel, Petr
1990LNP...363..279H    Altcode: 1990doqp.coll..279H; 1990IAUCo.117..279H
  No abstract at ADS

---------------------------------------------------------
Title: Chromospheric Structure under an H-alpha Filament
Authors: Heinzel, P.; Kononovich, E. V.; Smirnova, O. B.
1990PDHO....7..172H    Altcode: 1990dysu.conf..172H; 1990ESPM....6..172H
  The authors discuss the morphology and intensity structure of the
  chromosphere underlying the Hα filament located close to the solar
  limb.

---------------------------------------------------------
Title: Analysis of HeI 10830 a line in a quiescent prominence
Authors: Kotrč, P.; Heinzel, P.
1990LNP...363..285K    Altcode: 1990doqp.coll..285K; 1990IAUCo.117..285K
  No abstract at ADS

---------------------------------------------------------
Title: Hydrogen Lines Formation in Filamentary Prominences
Authors: Heinzel, P.
1989HvaOB..13..317H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Analysis of HeI 10830 Line in a Quiescent Prominence
Authors: Kotrc, P.; Heinzel, P.
1989HvaOB..13..371K    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Non LTE modelling of prominences.
Authors: Heinzel, P.; Gouttebroze, P.; Vial, J. -C.
1988dssp.conf...71H    Altcode:
  The authors present the results on non-LTE computations performed in
  the major lines and continua of the hydrogen atom. The prominence is
  represented by a slab illuminated by the neighbouring chromosphere and
  corona. Classical models are recomputed and it appears that the low
  pressure model represent well the observed Lα profiles. However the
  Lβ-computed value is much lower than the observed one. Preliminary
  computations where a transition region to the corona is included that
  the Lβ line may be improved.

---------------------------------------------------------
Title: Hα diagnostics of (post)-flare loops based on narrow-band
    filtergram observations
Authors: Heinzel, P.; Karlicky, M.
1987SoPh..110..343H    Altcode:
  Using narrow-band Hα filtergrams, we develop a quantitative
  non-LTE approach to determine the physical conditions prevailing
  at the tops of (post)-flare loops observed against the solar
  disc. At temperatures 10000-15000 K, the tops of flare loops turn
  to emission at Hα line center when the gas pressure P<SUB>g</SUB>
  reaches 1 dyn cm<SUP>−2</SUP> and should be clearly visible for
  P<SUB>g</SUB>≳ 3 dyn cm<SUP>−2</SUP>, independently of the
  loop diameter. This situation corresponds to the electron density
  of the order 10<SUP>12</SUP> cm<SUP>−3</SUP>. The contrast of
  flare-loops (in projection on the disc) at Hα line center is mainly
  the function of P<SUB>g</SUB>, while in the line wings (Hα ± 1 Å)
  the loop can be visible in absorption or emission only when rather
  strong microturbulence is present or for unrealistically high gas
  pressures. Finally, we briefly discuss our diagnostical results in
  frame of the latest (post)-flare loop model.

---------------------------------------------------------
Title: Formation of the hydrogen spectrum in quiescent prominences -
    One-dimensional models with standard partial redistribution
Authors: Heinzel, P.; Gouttebroze, P.; Vial, J. -C.
1987A&A...183..351H    Altcode:
  One-dimensional isothermal-isobaric static slab models are used to study
  departures from complete frequency redistribution (CRD) in hydrogen
  lines for quiescent solar prominences. Partial redistribution (PRD)
  effects on the hydrogen L-alpha line are shown to be significant
  in the near wings in addition to the far wings of L-alpha. It is
  suggested that strong symmetrical peaks found in the theoretical
  PRD L-alpha profiles are due to partially coherent penetration of
  the incidence double-peaked solar L-alpha. The present results are
  found to be consistent with OSO-8/LPSP observations and with UVSP/SMM
  data. The possible interplay between the effects of lateral transport
  or radiation, level-interlocking, and PRD is considered.

---------------------------------------------------------
Title: Book review
Authors: Heinzel, Petr
1987SoPh..110..411H    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Hydrogen Emission from Moving Solar Prominences
Authors: Heinzel, P.; Rompolt, B.
1987SoPh..110..171H    Altcode:
  Brightness variations of the lines arising from a five-level hydrogen
  model atom, depending upon prominence velocities, have been investigated
  using a combination of two non-LTE techniques. The importance of the
  Doppler brightening and/or Doppler dimming effects is demonstrated
  for the lines of the Lyman and Balmer series.

---------------------------------------------------------
Title: Optical and infrared spectrophotometry of quiescent
    prominences.
Authors: Novocky, D.; Heinzel, P.
1987PAICz..66..257N    Altcode: 1987eram....1..257N
  High-dispersion Ca II H and K, Ca II IR λ8542 Å, Hα, Hβ, and
  D<SUB>3</SUB> emission line profiles of quiescent prominences have
  been recorded in Stará Lesná Observatory. After data reduction,
  a full set of calibrated profiles is used to discuss semiempirical
  non-LTE prominence models.

---------------------------------------------------------
Title: Non-Lte Modelling of Prominences
Authors: Heinzel, P.; Gouttebroze, P.; Vial, J. C.
1987dssp.work...71H    Altcode: 1987ASSL..150...71H
  No abstract at ADS

---------------------------------------------------------
Title: Physical conditions in cool flare loops.
Authors: Heinzel, P.
1987PAICz..66..199H    Altcode: 1987eram....1..199H
  Large two-ribbon flares are frequently accompanied by a system of
  (post)-flare loops, cooler structures being visible in several optical
  and UV lines. The author investigates the non-LTE formation of hydrogen
  lines in stationary loop structures, taking into account the influence
  of macroscopic velocity flows along the loop.

---------------------------------------------------------
Title: Non-LTE hydrogen-line formation in moving prominences.
Authors: Heinzel, P.; Rompolt, B.
1986NASCP2442..163H    Altcode: 1986copp.nasa..163H
  The behavior of hydrogen-line brightness variations, depending on the
  prominence-velocity changes were investigated. By solving the NON-Local
  thermodynamic equilibrium (LTE) problem for hydrogen researchers
  determine quantitatively the effect of Doppler brightening and/or
  Doppler dimming (DBE, DDE) in the lines of Lyman and Balmer series. It
  is demonstrated that in low-density prominence plasmas, DBE in H alpha
  and H beta lines can reach a factor of three for velocities around 160
  km/sec, while the L alpha line exhibits typical DDE. L beta brightness
  variations follow from a combined DBE in the H alpha and DDE in L alpha
  and L beta itself, providing that all relevant multilevel interlocking
  processes are taken into account.

---------------------------------------------------------
Title: Partial redistribution effects in the formation of hydrogen
    lines in quiescent prominences.
Authors: Heinzel, P.; Gouttebroze, P.; Vial, J. C.
1986NASCP2442..155H    Altcode: 1986copp.nasa..155H
  Departures from complete frequency redistribution (CRD) in hydrogen
  lines are investigated for solar prominences. Partial redistribution
  effects (PRD) are found both in the wings (their already known lowering)
  and in the central part of the L alpha line; a new feature is evidenced
  here: the partially coherent scattering in the near wings of the
  line leads to a double-peaked profile mirroring the incident solar
  radiation. With a low density model, we obtain a good agreement with
  OSO 8 observed profiles. On the contrary, the PRD computed L beta
  profile (lower density, no reversal) departs from the observed one,
  a result which calls for more progress in terms of non-LTE transfer
  and modelling.

---------------------------------------------------------
Title: Comments on "The angle-dependent redistribution functions
    R<SUB>III</SUB> and R<SUB>IV</SUB>" by S. J. McKenna.
Authors: Hubeny, I.; Heinzel, P.
1986Ap&SS.119..409H    Altcode:
  It is shown that the complicated form of the line absorption probability
  function for scattering in subordinate lines, derived by McKenna (1984),
  is an artifact of adopting a mathematically inconvenient expression
  for the corresponding redistribution function. It is demonstrated that
  the absorption probability must be given by the Voigt function.

---------------------------------------------------------
Title: Non-LTE models of solar prominences
Authors: Heinzel, P.; Vial, J. C.; Gouttebroze, P.; Rompolt, B.
1986CoSka..15..183H    Altcode:
  The authors briefly review some representative non-LTE models of solar
  prominences, developed during the past decade. Particular attention is
  devoted to recent interpretation of hydrogen Lyman α line profiles
  in quiescent prominences and to the solution of the non-LTE problem
  for moving active prominences. Finally, the authors outline some of
  the most important prospects of prominence plasma diagnostics.

---------------------------------------------------------
Title: Infrared observations of quiescent prominences
Authors: Heinzel, P.; Kotrč, P.; Sobotka, M.; Zloch, F.; Scherbakova,
   Z. A.
1986CoSka..15..171H    Altcode:
  The authors have developed a sophisticated numerical technique to
  reduce infrared photographic spectra of quiescent prominences, taking
  into account the influence of instrumental profiles, scattered light
  and the noise. The reduced profiles were subsequently compared with
  theoretical ones.

---------------------------------------------------------
Title: Partial redistribution interlocking in the solar chromosphere.
Authors: Heinzel, P.; Hubeny, I.
1985ASIC..152..137H    Altcode: 1985pssl.proc..137H
  Starting with the model of a quiet solar chromosphere, the authors
  have calculated the relative probabilities of radiative and natural
  population of the second and third hydrogen levels, pertinent to
  various population processes. The analysis indicates that, while the Lα
  line is formed by resonance scattering between the first two levels,
  the third hydrogen level, from which Lβ and Hα are generated,
  is populated partly by direct photoexcitation 1→3 (about 55%),
  and partly by two-photon absorption 1→2→3 (about 45%).

---------------------------------------------------------
Title: Redistribution functions: a review of computational methods.
Authors: Heinzel, P.
1985ASIC..152..115H    Altcode: 1985pssl.proc..115H
  This paper reviews and compares the existing computational methods
  developed to evaluate various types of redistribution functions
  applicable in astrophysics. It discusses in detail several numerical
  aspects (codes) of calculating both the angle-dependent and
  angle-averaged laboratory-frame functions.

---------------------------------------------------------
Title: Non-coherent scattering in subordinate lines - V. Solutions
    of the transfer problem.
Authors: Hubeny, I.; Heinzel, P.
1984JQSRT..32..159H    Altcode:
  Redistribution functions are defined for resonance scattering and shown
  to be of use in astrophysics problems. An isotropic approximation is
  included in a definition of a two-level atom line source function and
  the redistribution function is angle-averaged for scattered photons,
  which are treated as negative absorption. Various redistribution
  functions, either partial or complete, are then applied to slab,
  isothermal, finite, and semi-infinite atmospheres for a given absorption
  profile and the line source function to examine the resulting transfer
  functions. The ratios of the upper/lower level damping are found to
  have a significant impact on the type of redistribution expected. An
  approximate form of the redistribution function is determined as
  adequate for calculating line profiles, especially in the wings.

---------------------------------------------------------
Title: Non-coherent scattering in subordinate lines:
    IV. Angle-averaged redistribution functions.
Authors: Heinzel, P.; Hubený, I.
1983JQSRT..30...77H    Altcode:
  It is demonstrated that a simple Gaussian quadrature over the
  scattering angles provides a sufficiently accurate and stable method
  for evaluating all the angle-averaged redistribution functions
  R<SUB>i</SUB>(xarcmin,x) (i = I-V). The authors display graphically
  the functions R<SUB>II,III,V</SUB> and discuss in detail the behaviour
  of the newly calculated redistribution R<SUB>V</SUB>(xarcmin,x).

---------------------------------------------------------
Title: OSO-8 observations of a quiescent prominence - A comparison
    of Lyman-alpha with theoretical intensities
Authors: Heinzel, P.; Vial, J. -C.
1983A&A...121..155H    Altcode:
  Using simultaneous observations of hydrogen Lyman-α and Ca II K lines
  obtained with the OSO 8 LPSP instrument, the authors compare Lα
  emission from a quiescent prominence with those predicted from the
  existing theoretical models. They use the observed relation between
  Hα and Ca II K integrated intensities to obtain an estimate of
  E(Hα)/E(Lα) vs. E(Hα). This ratio differs significantly from those
  predicted theoretically under the assumption of complete frequency
  redistribution during the scattering of Lα photons. On the other
  hand, using the partial-redistribution treatment in the Lα wings,
  as suggested by Milkey et al., the authors arrived at a reasonable
  agreement with the corresponding theoretical curve. The possible
  influence of macroscopic velocities on line ratios is briefly discussed.

---------------------------------------------------------
Title: Resonance Scattering of Radiation in Solar
    Prominences. I. Partial Redistribution in Optically Thin Subordinate
    Lines
Authors: Heinzel, P.
1983BAICz..34....1H    Altcode:
  In the present paper the author studies the resonance scattering of
  photospheric and chromospheric radiation by a prominence located at
  any given height above the solar surface. Applying the newly developed
  partial redistribution treatment (PRD), he evaluates numerically
  the scattering integral in order to assess possible PRD effects on
  subordinate-line emission profiles and/or integrated intensities
  emerging from an optically thin prominence plasma.

---------------------------------------------------------
Title: Book-Review - Laser Spectroscopy - Basic Concepts and
    Instrumentation
Authors: Demtroder, W.; Heinzel, P.
1982BAICz..33..192D    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Nekoherentní rozptyl záření v subordinátních čarách

---------------------------------------------------------
Title: Nekoherentní rozptyl záření v subordinátních čarách
Authors: Heinzel, Petr
1982PhDT.......141H    Altcode:
  No abstract at ADS

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Title: Erratum: "Non-coherent scattering in subordinate
lines: a unified approach to redistributions"
    [J. Quant. Spectrosc. Radiat. Transfer, Vol. 25, p. 483 - 499 (1981)].
Authors: Heinzel, P.
1982JQSRT..27..109H    Altcode:
  No abstract at ADS

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Title: Non-coherent scattering in subordinate lines: II. Collisional
    redistribution.
Authors: Heinzel, P.; Hubený, I.
1982JQSRT..27....1H    Altcode:
  No abstract at ADS

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Title: Partial frequency redistribution in subordinate lines.
Authors: Heinzel, P.
1981PAICz..57....5H    Altcode:
  No abstract at ADS

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Title: Non-coherent scattering in subordinate lines: a unified
    approach to redistribution functions.
Authors: Heinzel, P.
1981JQSRT..25..483H    Altcode:
  No abstract at ADS

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Title: Book-Review - Nonradial and Nonlinear Stellar Pulsation -
    Workshop - Tucson - 1979MAR12-16
Authors: Hill, H. A.; Dziembowski, W. A.; Heinzel, P.
1981BAICz..32..254H    Altcode:
  No abstract at ADS

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Title: Conference on stellar atmospheres, June 1981, Brno.
Authors: Heinzel, P.
1981Rise...62..203H    Altcode:
  No abstract at ADS

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Title: Partial frequency redistribution in subordinate lines
Authors: Heinzel, P.
1981sspi.book....5H    Altcode:
  An appropriate laboratory-frame redistribution function (LFR)
  subordinate lines formed in stellar atmospheres and solar prominences
  is presented under the assumption of a Maxwellian velocity distribution
  for the lower state atoms. Starting from quantum mechanical results. A
  LFR is obtained for the case of radiative broadening of both levels. One
  general routine that can be used to evaluate all is R sub IS.

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Title: Derivatives of the Voigt Functions
Authors: Heinzel, P.
1978BAICz..29..159H    Altcode:
  A procedure for computing the partial derivatives of the Voigt functions
  H(a, u) and K(a, u) is set forth, based on introducing the complex
  function D(w) = H(a, u) + iK(a, u). Recurrence relations for the partial
  derivatives up to the n-th order with respect to the variables a and
  u are derived. The direct formulas for these derivatives up to third
  order are also given. As an example of an astrophysical application,
  the expression for a hydrogen line profile as a linear combination of
  the partial derivatives of a Voigt function is given.

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Title: Astronomy at the Jagellonian University.
Authors: Heinzel, P.
1976Rise...57...81H    Altcode:
  No abstract at ADS

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Title: Precise Measurements of Radial Velocity Using a Lirepho
    Microphotometer
Authors: Heinzel, P.; Hadrava, P.
1975BAICz..26...90H    Altcode:
  No abstract at ADS

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Title: European seminary of the students of astronomy in Poland, 1973.
Authors: Heinzel, P.; Solc, M.
1974Rise...55...29H    Altcode:
  No abstract at ADS