Author name code: mariska ADS astronomy entries on 2022-09-14 author:"Mariska, John T." ------------------------------------------------------------------------ Title: Achievements of Hinode in the first eleven years Authors: Hinode Review Team; Al-Janabi, Khalid; Antolin, Patrick; Baker, Deborah; Bellot Rubio, Luis R.; Bradley, Louisa; Brooks, David H.; Centeno, Rebecca; Culhane, J. Leonard; Del Zanna, Giulio; Doschek, George A.; Fletcher, Lyndsay; Hara, Hirohisa; Harra, Louise K.; Hillier, Andrew S.; Imada, Shinsuke; Klimchuk, James A.; Mariska, John T.; Pereira, Tiago M. D.; Reeves, Katharine K.; Sakao, Taro; Sakurai, Takashi; Shimizu, Toshifumi; Shimojo, Masumi; Shiota, Daikou; Solanki, Sami K.; Sterling, Alphonse C.; Su, Yingna; Suematsu, Yoshinori; Tarbell, Theodore D.; Tiwari, Sanjiv K.; Toriumi, Shin; Ugarte-Urra, Ignacio; Warren, Harry P.; Watanabe, Tetsuya; Young, Peter R. Bibcode: 2019PASJ...71R...1H Altcode: Hinode is Japan's third solar mission following Hinotori (1981-1982) and Yohkoh (1991-2001): it was launched on 2006 September 22 and is in operation currently. Hinode carries three instruments: the Solar Optical Telescope, the X-Ray Telescope, and the EUV Imaging Spectrometer. These instruments were built under international collaboration with the National Aeronautics and Space Administration and the UK Science and Technology Facilities Council, and its operation has been contributed to by the European Space Agency and the Norwegian Space Center. After describing the satellite operations and giving a performance evaluation of the three instruments, reviews are presented on major scientific discoveries by Hinode in the first eleven years (one solar cycle long) of its operation. This review article concludes with future prospects for solar physics research based on the achievements of Hinode. Title: Comprehensive Determination of the Hinode/EIS Roll Angle Authors: Pelouze, Gabriel; Auchère, Frédéric; Bocchialini, Karine; Harra, Louise; Baker, Deborah; Warren, Harry P.; Brooks, David H.; Mariska, John T. Bibcode: 2019SoPh..294...59P Altcode: 2019arXiv190311923P We present a new coalignment method for the EUV Imaging Spectrometer (EIS) on board the Hinode spacecraft. In addition to the pointing offset and spacecraft jitter, this method determines the roll angle of the instrument, which has never been systematically measured, and which is therefore usually not corrected. The optimal pointing for EIS is computed by maximizing the cross-correlations of the Fe XII 195.119 Å line with images from the 193 Å band of the Atmospheric Imaging Assembly (AIA) on board the Solar Dynamics Observatory (SDO). By coaligning 3336 rasters with high signal-to-noise ratio, we estimate the rotation angle between EIS and AIA and explore the distribution of its values. We report an average value of (−0.387±0.007 ) ∘. We also provide a software implementation of this method that can be used to coalign any EIS raster. Title: A Tale of Two Books Authors: Mariska, John Bibcode: 2016S&T...132c..86M Altcode: No abstract at ADS Title: Progress toward high resolution EUV spectroscopy Authors: Korendyke, C.; Doschek, G. A.; Warren, H.; Young, P. R.; Chua, D.; Hassler, D. M.; Landi, E.; Davila, J. M.; Klimchuck, J.; Tun, S.; DeForest, C.; Mariska, J. T.; Solar C Spectroscopy Working Group; LEMUR; EUVST Development Team Bibcode: 2013SPD....44..143K Altcode: HIgh resolution EUV spectroscopy is a critical instrumental technique to understand fundamental physical processes in the high temperature solar atmosphere. Spectroscopic observations are used to measure differential emission measure, line of sight and turbulent flows, plasma densities and emission measures. Spatially resolved, spectra of these emission lines with adequate cadence will provide the necessary clues linking small scale structures with large scale, energetic solar phenomena. The necessary observations to determine underlying physical processes and to provide comprehensive temperature coverage of the solar atmosphere above the chromosphere will be obtained by the proposed EUVST instrument for Solar C. This instrument and its design will be discussed in this paper. Progress on the VEry high Resolution Imaging Spectrograph (VERIS) sounding rocket instrument presently under development at the Naval Research Laboratory will also be discussed. Title: Observations of Thermal Flare Plasma with the EUV Variability Experiment Authors: Warren, Harry P.; Mariska, John T.; Doschek, George A. Bibcode: 2013ApJ...770..116W Altcode: 2012arXiv1211.1875W One of the defining characteristics of a solar flare is the impulsive formation of very high temperature plasma. The properties of the thermal emission are not well understood, however, and the analysis of solar flare observations is often predicated on the assumption that the flare plasma is isothermal. The EUV Variability Experiment (EVE) on the Solar Dynamics Observatory provides spectrally resolved observations of emission lines that span a wide range of temperatures (e.g., Fe XV-Fe XXIV) and allow for thermal flare plasma to be studied in detail. In this paper we describe a method for computing the differential emission measure distribution in a flare using EVE observations and apply it to several representative events. We find that in all phases of the flare the differential emission measure distribution is broad. Comparisons of EVE spectra with calculations based on parameters derived from the Geostationary Operational Environmental Satellites soft X-ray fluxes indicate that the isothermal approximation is generally a poor representation of the thermal structure of a flare. Title: On-Orbit Sensitivity Evolution of the EUV Imaging Spectrometer on Hinode Authors: Mariska, J. T. Bibcode: 2013SoPh..282..629M Altcode: 2012arXiv1211.3694M Since its launch on 22 September 2006, the EUV Imaging Spectrometer onboard the Hinode satellite has exhibited a gradual decay in sensitivity. Using spectroheliograms taken in the Fe VIII 185.21 Å and Si VII 275.35 Å emission lines in quiet regions near Sun center we characterize that decay. For the period from December 2006 to March 2012, the decline in the sensitivity can be characterized as an exponential decay with an average time constant of 7358±1030 days (20.2±2.8 years). Emission lines formed at temperatures ≳ 106.1 K in the quiet Sun data exhibit solar-cycle effects. Title: LEMUR: Large European module for solar Ultraviolet Research. European contribution to JAXA's Solar-C mission Authors: Teriaca, Luca; Andretta, Vincenzo; Auchère, Frédéric; Brown, Charles M.; Buchlin, Eric; Cauzzi, Gianna; Culhane, J. Len; Curdt, Werner; Davila, Joseph M.; Del Zanna, Giulio; Doschek, George A.; Fineschi, Silvano; Fludra, Andrzej; Gallagher, Peter T.; Green, Lucie; Harra, Louise K.; Imada, Shinsuke; Innes, Davina; Kliem, Bernhard; Korendyke, Clarence; Mariska, John T.; Martínez-Pillet, Valentin; Parenti, Susanna; Patsourakos, Spiros; Peter, Hardi; Poletto, Luca; Rutten, Robert J.; Schühle, Udo; Siemer, Martin; Shimizu, Toshifumi; Socas-Navarro, Hector; Solanki, Sami K.; Spadaro, Daniele; Trujillo-Bueno, Javier; Tsuneta, Saku; Dominguez, Santiago Vargas; Vial, Jean-Claude; Walsh, Robert; Warren, Harry P.; Wiegelmann, Thomas; Winter, Berend; Young, Peter Bibcode: 2012ExA....34..273T Altcode: 2011ExA...tmp..135T; 2011arXiv1109.4301T The solar outer atmosphere is an extremely dynamic environment characterized by the continuous interplay between the plasma and the magnetic field that generates and permeates it. Such interactions play a fundamental role in hugely diverse astrophysical systems, but occur at scales that cannot be studied outside the solar system. Understanding this complex system requires concerted, simultaneous solar observations from the visible to the vacuum ultraviolet (VUV) and soft X-rays, at high spatial resolution (between 0.1'' and 0.3''), at high temporal resolution (on the order of 10 s, i.e., the time scale of chromospheric dynamics), with a wide temperature coverage (0.01 MK to 20 MK, from the chromosphere to the flaring corona), and the capability of measuring magnetic fields through spectropolarimetry at visible and near-infrared wavelengths. Simultaneous spectroscopic measurements sampling the entire temperature range are particularly important. These requirements are fulfilled by the Japanese Solar-C mission (Plan B), composed of a spacecraft in a geosynchronous orbit with a payload providing a significant improvement of imaging and spectropolarimetric capabilities in the UV, visible, and near-infrared with respect to what is available today and foreseen in the near future. The Large European Module for solar Ultraviolet Research (LEMUR), described in this paper, is a large VUV telescope feeding a scientific payload of high-resolution imaging spectrographs and cameras. LEMUR consists of two major components: a VUV solar telescope with a 30 cm diameter mirror and a focal length of 3.6 m, and a focal-plane package composed of VUV spectrometers covering six carefully chosen wavelength ranges between 170 Å and 1270 Å. The LEMUR slit covers 280'' on the Sun with 0.14'' per pixel sampling. In addition, LEMUR is capable of measuring mass flows velocities (line shifts) down to 2 km s - 1 or better. LEMUR has been proposed to ESA as the European contribution to the Solar C mission. Title: Long-Term Variation of the Corona in Quiet Regions Authors: Kamio, S.; Mariska, J. T. Bibcode: 2012SoPh..279..419K Altcode: 2012arXiv1204.5575K Using Hinode EUV Imaging Spectrometer (EIS) spectra recorded daily at Sun center from the end of 2006 to early 2011, we studied the long-term evolution of the quiet corona. The light curves of the higher temperature emission lines exhibit larger variations in sync with the solar activity cycle while the cooler lines show reduced modulation. Our study shows that the high temperature component of the corona changes in quiet regions, even though the coronal electron density remains almost constant there. The results suggest that heat input to the quiet corona varies with the solar activity cycle. Title: Coupling of Particle Acceleration and Atmospheric Dynamic Response to Impulsive Energy Release in Solar Flares Authors: Liu, Wei; Petrosian, V.; Chen, Q.; Mariska, J. Bibcode: 2012AAS...22020419L Altcode: In solar flares, acceleration and transport of high-energy particles and fluid dynamics of the atmospheric plasma are interrelated processes coupled in a circular chain. Chromospheric evaporation, for example, can alter the density and temperature distribution along the flare loop, in particular in the acceleration site near the loop-top source. This produces a feedback on particle collisional heating, and more importantly on the energy release and acceleration process. This in turn will change the heating of the chromosphere and mass flows in the corona. In recent years, there have been increasing theoretical and observational motivations to investigate these coupled processes together in a self-consistent manner. We present here combined Fokker-­Planck modeling of particles and hydrodynamic simulation of flare plasma. We extended our earlier hybrid simulation (Liu, Petrosian, Mariska 2009) by feeding the updated plasma density and temperature at the loop-top source to the stochastic acceleration process. We find that the density enhancement causes the ratio of the electron plasma frequency to gyro-frequency to increase. This can lead to the reduction of the efficiency of electron acceleration and thus the quenching or spectral softening of nonthermal hard X-ray tails observed during the late stages of flares. This also affects the relative production of energetic electrons vs. protons (Petrosian and Liu 2004). We will compare our results with recent observations from RHESSI, SDO, and Hinode. We will also discuss their implications for cyclic spectral hardening, quasi-periodic flare pulsations, and recently imaged super-fast quasi-periodic coronal waves originating from flare kernels. Title: Extreme Ultraviolet Variability Experiment (EVE) on the Solar Dynamics Observatory (SDO): Overview of Science Objectives, Instrument Design, Data Products, and Model Developments Authors: Woods, T. N.; Eparvier, F. G.; Hock, R.; Jones, A. R.; Woodraska, D.; Judge, D.; Didkovsky, L.; Lean, J.; Mariska, J.; Warren, H.; McMullin, D.; Chamberlin, P.; Berthiaume, G.; Bailey, S.; Fuller-Rowell, T.; Sojka, J.; Tobiska, W. K.; Viereck, R. Bibcode: 2012SoPh..275..115W Altcode: The highly variable solar extreme ultraviolet (EUV) radiation is the major energy input to the Earth's upper atmosphere, strongly impacting the geospace environment, affecting satellite operations, communications, and navigation. The Extreme ultraviolet Variability Experiment (EVE) onboard the NASA Solar Dynamics Observatory (SDO) will measure the solar EUV irradiance from 0.1 to 105 nm with unprecedented spectral resolution (0.1 nm), temporal cadence (ten seconds), and accuracy (20%). EVE includes several irradiance instruments: The Multiple EUV Grating Spectrographs (MEGS)-A is a grazing-incidence spectrograph that measures the solar EUV irradiance in the 5 to 37 nm range with 0.1-nm resolution, and the MEGS-B is a normal-incidence, dual-pass spectrograph that measures the solar EUV irradiance in the 35 to 105 nm range with 0.1-nm resolution. To provide MEGS in-flight calibration, the EUV SpectroPhotometer (ESP) measures the solar EUV irradiance in broadbands between 0.1 and 39 nm, and a MEGS-Photometer measures the Sun's bright hydrogen emission at 121.6 nm. The EVE data products include a near real-time space-weather product (Level 0C), which provides the solar EUV irradiance in specific bands and also spectra in 0.1-nm intervals with a cadence of one minute and with a time delay of less than 15 minutes. The EVE higher-level products are Level 2 with the solar EUV irradiance at higher time cadence (0.25 seconds for photometers and ten seconds for spectrographs) and Level 3 with averages of the solar irradiance over a day and over each one-hour period. The EVE team also plans to advance existing models of solar EUV irradiance and to operationally use the EVE measurements in models of Earth's ionosphere and thermosphere. Improved understanding of the evolution of solar flares and extending the various models to incorporate solar flare events are high priorities for the EVE team. Title: New Solar Extreme-ultraviolet Irradiance Observations during Flares Authors: Woods, Thomas N.; Hock, Rachel; Eparvier, Frank; Jones, Andrew R.; Chamberlin, Phillip C.; Klimchuk, James A.; Didkovsky, Leonid; Judge, Darrell; Mariska, John; Warren, Harry; Schrijver, Carolus J.; Webb, David F.; Bailey, Scott; Tobiska, W. Kent Bibcode: 2011ApJ...739...59W Altcode: New solar extreme-ultraviolet (EUV) irradiance observations from the NASA Solar Dynamics Observatory (SDO) EUV Variability Experiment provide full coverage in the EUV range from 0.1 to 106 nm and continuously at a cadence of 10 s for spectra at 0.1 nm resolution and even faster, 0.25 s, for six EUV bands. These observations can be decomposed into four distinct characteristics during flares. First, the emissions that dominate during the flare's impulsive phase are the transition region emissions, such as the He II 30.4 nm. Second, the hot coronal emissions above 5 MK dominate during the gradual phase and are highly correlated with the GOES X-ray. A third flare characteristic in the EUV is coronal dimming, seen best in the cool corona, such as the Fe IX 17.1 nm. As the post-flare loops reconnect and cool, many of the EUV coronal emissions peak a few minutes after the GOES X-ray peak. One interesting variation of the post-eruptive loop reconnection is that warm coronal emissions (e.g., Fe XVI 33.5 nm) sometimes exhibit a second large peak separated from the primary flare event by many minutes to hours, with EUV emission originating not from the original flare site and its immediate vicinity, but rather from a volume of higher loops. We refer to this second peak as the EUV late phase. The characterization of many flares during the SDO mission is provided, including quantification of the spectral irradiance from the EUV late phase that cannot be inferred from GOES X-ray diagnostics. Title: Physical Properties of Solar Flares: New Results from EVE/SDO Authors: Warren, H. P.; Mariska, J. T.; Doschek, G. A.; Eve Team Bibcode: 2010AGUFMSH13A..06W Altcode: Much of our current understanding of the temperature and density structure of solar flares has been derived from broad band X-ray instruments, such as RHESSI, GOES, and SXT/Yohkoh, or the observation of isolated emission lines, such as from BCS/Yohkoh. This has lead to uncertainties in determining the distribution of temperatures and densities in a flare. The EUV Variability Experiment (EVE) on the Solar Dynamics Observatory (SDO) provides an unprecedented opportunity to observe a very wide range of high-temperature emission lines at high cadence (10 s) and relatively high spectral resolution (1 A). The spectral range between 90 and 200 Angstroms is particularly rich in emission lines from Fe that are formed at temperatures above 7 MK (Fe XVIII - Fe XXIV). This range also includes one of the few density diagnostics (Fe XXI 145.66/128.75) that is useful in solar flare observations. Our initial calculations suggest very broad differential emission measure distributions and indicate high densities (Log Ne as high as 11.7), which implies a very rapid cooling of flare plasma. These observations are broadly consistent with flare models that allow for the release of energy on many independent threads and we will discuss these results in the context of current theories of solar flares. Title: Science Objectives for an X-Ray Microcalorimeter Observing the Sun Authors: Laming, J. Martin; Adams, J.; Alexander, D.; Aschwanden, M; Bailey, C.; Bandler, S.; Bookbinder, J.; Bradshaw, S.; Brickhouse, N.; Chervenak, J.; Christe, S.; Cirtain, J.; Cranmer, S.; Deiker, S.; DeLuca, E.; Del Zanna, G.; Dennis, B.; Doschek, G.; Eckart, M.; Fludra, A.; Finkbeiner, F.; Grigis, P.; Harrison, R.; Ji, L.; Kankelborg, C.; Kashyap, V.; Kelly, D.; Kelley, R.; Kilbourne, C.; Klimchuk, J.; Ko, Y. -K.; Landi, E.; Linton, M.; Longcope, D.; Lukin, V.; Mariska, J.; Martinez-Galarce, D.; Mason, H.; McKenzie, D.; Osten, R.; Peres, G.; Pevtsov, A.; Porter, K. Phillips F. S.; Rabin, D.; Rakowski, C.; Raymond, J.; Reale, F.; Reeves, K.; Sadleir, J.; Savin, D.; Schmelz, J.; Smith, R. K.; Smith, S.; Stern, R.; Sylwester, J.; Tripathi, D.; Ugarte-Urra, I.; Young, P.; Warren, H.; Wood, B. Bibcode: 2010arXiv1011.4052L Altcode: We present the science case for a broadband X-ray imager with high-resolution spectroscopy, including simulations of X-ray spectral diagnostics of both active regions and solar flares. This is part of a trilogy of white papers discussing science, instrument (Bandler et al. 2010), and missions (Bookbinder et al. 2010) to exploit major advances recently made in transition-edge sensor (TES) detector technology that enable resolution better than 2 eV in an array that can handle high count rates. Combined with a modest X-ray mirror, this instrument would combine arcsecondscale imaging with high-resolution spectra over a field of view sufficiently large for the study of active regions and flares, enabling a wide range of studies such as the detection of microheating in active regions, ion-resolved velocity flows, and the presence of non-thermal electrons in hot plasmas. It would also enable more direct comparisons between solar and stellar soft X-ray spectra, a waveband in which (unusually) we currently have much better stellar data than we do of the Sun. Title: SDO Extreme Ultraviolet Variability Experiment (EVE): Instrument and First Light Authors: Woods, Thomas N.; Eparvier, F.; Hock, R.; Jones, A.; Didkovsky, L.; Judge, D.; Chamberlin, P.; Lean, J.; Warren, H.; Mariska, J. Bibcode: 2010AAS...21630802W Altcode: The Extreme ultraviolet Variability Experiment (EVE) aboard the NASA Solar Dynamics Observatory (SDO) was launched on 11 February 2010. The EVE instruments measure the solar extreme ultraviolet (EUV) irradiance from 0.1 to 105 nm with unprecedented spectral resolution (0.1 nm), temporal cadence (10 sec minimum), and accuracy (20% or better). The highly variable solar EUV irradiance is a key measurement for the NASA Living With the Star (LWS) program as it is the major energy input into the Earth's upper atmosphere and thus impacts the geospace environment that affects satellite operations and communication and navigation systems. The EVE measurements, along with additional solar measurements from SDO and other satellite and ground-based instruments, will be used to advance our understanding of the solar EUV irradiance variability. For short time scales, EVE will make detailed observations on the evolution of flare events that are an important interest for space weather research and operations. For longer time scales, EVE measurements will be compared to other solar EUV irradiance measurements to help establish a composite time series of the solar EUV irradiance. The EVE instrument will be described, and first light results from EVE during the rise of solar cycle 24 will be presented. The EVE instrument team is supported by the NASA SDO Project. Title: Doppler-shift, Intensity, and Density Oscillations Observed with the Extreme Ultraviolet Imaging Spectrometer on Hinode Authors: Mariska, John T.; Muglach, K. Bibcode: 2010ApJ...713..573M Altcode: 2010arXiv1003.0420M Low-amplitude Doppler-shift oscillations have been observed in coronal emission lines in a number of active regions with the EUV Imaging Spectrometer (EIS) on the Hinode satellite. Both standing and propagating waves have been detected and many periods have been observed, but a clear picture of all the wave modes that might be associated with active regions has not yet emerged. In this study, we examine additional observations obtained with EIS in plage near an active region on 2007 August 22-23. We find Doppler-shift oscillations with amplitudes between 1 and 2 km s-1 in emission lines ranging from Fe XI 188.23 Å, which is formed at log T = 6.07, to Fe XV 284.16 Å, which is formed at log T = 6.32. Typical periods are near 10 minutes. We also observe intensity and density oscillations for some of the detected Doppler-shift oscillations. In the better-observed cases, the oscillations are consistent with upwardly propagating slow magnetoacoustic waves. Simultaneous observations of the Ca II H line with the Hinode Solar Optical Telescope Broadband Filter Imager show some evidence for 10 minute oscillations as well. Title: Doppler Shift Oscillations Observed with the EUV Imaging Spectrometer on Hinode Authors: Mariska, J. T. Bibcode: 2009ASPC..415..283M Altcode: This contribution reports on the detection of Doppler-shift oscillations in an active region observed on 2007 August 22-23. The oscillations, which have a much lower amplitude than those observed with earlier instruments, have periods of 7 to 10 min. These observations include density-sensitive emission lines and oscillations are also present in the derived densities. EIS is capable of detecting coronal velocity fluctuations with amplitudes of less than 0.5 km s-1 with short integration times in strong coronal lines, potentially allowing access to a much richer range of coronal oscillatory phenomena than has been available with earlier instruments. Title: The Second Hinode Science Meeting: Beyond Discovery-Toward Understanding Authors: Lites, B.; Cheung, M.; Magara, T.; Mariska, J.; Reeves, K. Bibcode: 2009ASPC..415.....L Altcode: No abstract at ADS Title: Combined Fokker-Planck Modeling of Particle Acceleration/Transport and Hydrodynamic Simulation of Atmospheric Response in Solar Flares Authors: Petrosian, V.; Liu, W.; Mariska, J. T. Bibcode: 2009AGUFMSH21C..04P Altcode: Acceleration and transport of high-energy particles and fluid dynamics of atmospheric plasma are interrelated aspects of solar flares, but for simplicity they were artificially separated in the past. We present here self-consistently combined Fokker-Planck modeling of particles and hydrodynamic simulation of flare plasma. Energetic electrons are modeled with the Stanford unified code of acceleration, transport, and radiation, while plasma is modeled with the NRL flux tube code (Mariska et al. 1989). We calculated the collisional heating rate directly from the particle transport code, which is more accurate than those in previous studies based on approximate analytical solutions. We used a more realistic spectrum of injected electrons provided by the stochastic acceleration model of Petrosian & Liu (2004), which has a smooth transition from a quasi-thermal background at low energies to a nonthermal tail at high energies. The inclusion of low-energy electrons results in relatively more heating in the corona (vs. chromosphere) and thus a larger downward heat conduction flux. The interplay of electron heating, conduction, and radiative loss leads to stronger chromospheric evaporation than obtained in previous studies, which had a deficit in low-energy electrons due to an arbitrarily assumed low-energy cutoff. The energy and spatial distributions of energetic electrons and bremsstrahlung photons bear signatures of the changing density distribution caused by chromospheric evaporation. In particular, the density jump at the evaporation front gives rise to enhanced X-ray emission, which could be responsible for the X-ray sources moving along flare loops observed by RHESSI (Sui et al. 2006, ApJL 645; Liu et al. 2006, ApJ 649). Various energy contents from the simulations can be used to test the empirical Neupert effect. This technique can also be applied to investigate a variety of high-energy processes in solar, space, and astrophysical plasmas, such as planetary auroras. Geometry of the model flare loop assumed in this study. Title: Hinode/EIS observations of propagating low-frequency slow magnetoacoustic waves in fan-like coronal loops Authors: Wang, T. J.; Ofman, L.; Davila, J. M.; Mariska, J. T. Bibcode: 2009A&A...503L..25W Altcode: 2009arXiv0908.0310W Aims: We report the first observation of multiple-periodic propagating disturbances along a fan-like coronal structure simultaneously detected in both intensity and Doppler shift in the Fe xii 195 Å line with the EUV Imaging Spectrometer (EIS) onboard Hinode. A new application of coronal seismology is provided based on this observation.
Methods: We analyzed the EIS sit-and-stare mode observation of oscillations using the running difference and wavelet techniques.
Results: Two harmonics with periods of 12 and 25 min are detected. We measured the Doppler shift amplitude of 1-2 km s-1, the relative intensity amplitude of 3%-5% and the apparent propagation speed of 100-120 km s-1.
Conclusions: The amplitude relationship between intensity and Doppler shift oscillations provides convincing evidence that these propagating features are a manifestation of slow magnetoacoustic waves. Detection lengths (over which the waves are visible) of the 25 min wave are about 70-90 Mm, much longer than those of the 5 min wave previously detected by TRACE. This difference may be explained by the dependence of damping length on the wave period for thermal conduction. Based on a linear wave theory, we derive an inclination of the magnetic field to the line-of-sight about 59 ± 8°, a true propagation speed of 128 ± 25 km s-1 and a temperature of 0.7 ± 0.3 MK near the loop's footpoint from our measurements.

Appendix is only available in electronic form at http://www.aanda.org Title: Combined Modeling of Acceleration, Transport, and Hydrodynamic Response in Solar Flares. I. The Numerical Model Authors: Liu, Wei; Petrosian, Vahé; Mariska, John T. Bibcode: 2009ApJ...702.1553L Altcode: 2009arXiv0906.2449L Acceleration and transport of high-energy particles and fluid dynamics of atmospheric plasma are interrelated aspects of solar flares, but for convenience and simplicity they were artificially separated in the past. We present here self-consistently combined Fokker-Planck modeling of particles and hydrodynamic simulation of flare plasma. Energetic electrons are modeled with the Stanford unified code of acceleration, transport, and radiation, while plasma is modeled with the Naval Research Laboratory flux tube code. We calculated the collisional heating rate directly from the particle transport code, which is more accurate than those in previous studies based on approximate analytical solutions. We repeated the simulation of Mariska et al. with an injection of power law, downward-beamed electrons using the new heating rate. For this case, a ~10% difference was found from their old result. We also used a more realistic spectrum of injected electrons provided by the stochastic acceleration model, which has a smooth transition from a quasi-thermal background at low energies to a nonthermal tail at high energies. The inclusion of low-energy electrons results in relatively more heating in the corona (versus chromosphere) and thus a larger downward heat conduction flux. The interplay of electron heating, conduction, and radiative loss leads to stronger chromospheric evaporation than obtained in previous studies, which had a deficit in low-energy electrons due to an arbitrarily assumed low-energy cutoff. The energy and spatial distributions of energetic electrons and bremsstrahlung photons bear signatures of the changing density distribution caused by chromospheric evaporation. In particular, the density jump at the evaporation front gives rise to enhanced emission, which, in principle, can be imaged by X-ray telescopes. This model can be applied to investigate a variety of high-energy processes in solar, space, and astrophysical plasmas. Title: Doppler Shift Oscillations Observed with the EUV Imaging Spectrometer on Hinode Authors: Mariska, John T.; Muglach, K. Bibcode: 2009SPD....40.1301M Altcode: The EUV Imaging Spectrometer (EIS) on Hinode is capable of measuring Doppler shift fluctuations with amplitudes of less than 0.5 km/s. This, coupled with EIS's improved sensitivity over previous EUV spectrometers, has expanded the range of coronal oscillatory phenomena available for detailed study. For example, both kink mode and slow mode coronal loop oscillations have already been detected with EIS. We report on additional observations of Doppler shift and intensity oscillations in an active region observed in 2007 August. An initial periodogram analysis of portions of the data shows periods in the Doppler shift data of 9 to 10 minutes in emission lines with temperatures of formation from 1.2 to 2.1 MK. Periods of 8 to 12 minutes are seen in the detrended intensity data over the same temperature range. The EIS observations include density-sensitive emission lines from Fe XII and Fe XIII, allowing us to quantify density fluctuations. The Solar Optical Telescope on Hinode made simultaneous Ca II observations, which we have co-aligned with the EIS data to understand better the chromospheric environment in the oscillating region.

This work was supported by the NASA Hinode program. Title: High-precision density measurements in the solar corona. I. Analysis methods and results for Fe XII and Fe XIII Authors: Young, P. R.; Watanabe, T.; Hara, H.; Mariska, J. T. Bibcode: 2009A&A...495..587Y Altcode: 2008arXiv0805.0958Y Aims: The EUV Imaging Spectrometer (EIS) instrument on board the Hinode satellite has access to some of the best coronal density diagnostics, and the high sensitivity of the instrument now allows electron number density, N_e, measurements to an unprecedented precision of up to ±5% in active regions. This paper gives a thorough overview of data analysis issues for the best diagnostics of Fe XII and Fe XIII and assesses the accuracy of the measurements.
Methods: Two density diagnostics each from Fe XII (λ186.88/λ195.12 and λ196.64/λ195.12) and Fe XIII (λ196.54/λ202.04 and λ203.82/λ202.04) are analysed in two active region datasets from 2007 May 3 and 6 that yield densities in the range 8.5≤ log (N_e/cm-3)≤ 11.0. The densities are derived using v5.2 of the CHIANTI atomic database. Blending, line fitting, and instrumental issues are discussed, and line fit parameters presented.
Results: The Fe XII and Fe XIII diagnostics show broadly the same trend in density across the active region, consistent with their similar temperatures of formation. However, the high precision of the EIS measurements demonstrates significant discrepancies of up to 0.5 dex in derived log Ne values, with Fe XII always giving higher densities than Fe XIII. The discrepancies may partly be due to real physical differences between the emitting regions of the two plasmas, but the dominant factor lies in the atomic models of the two ions. Two specific problems are identified for Fe XII λ196.64 and Fe XIII λ203.82: the former is found to be underestimated in strength by the CHIANTI atomic model, while the high-density limit of the λ203.82/λ202.04 ratio appears to be inaccurate in the CHIANTI atomic model. The small grating tilt of the EIS instrument is found to be very significant when deriving densities from emission lines separated by more than a few angstroms. Revised wavelengths of 196.518± 0.003 Å and 196.647± 0.003 Å are suggested for the Fe XIII λ196.54 and Fe XII λ196.64 lines, respectively. Title: Commission 12: Solar Radiation and Structure Authors: Martínez Pillet, Valentin; Kosovichev, Alexander; Mariska, John T.; Bogdan, Thomas J.; Asplund, Martin; Cauzzi, Gianna; Christensen-Dalsgaard, Jørgen; Cram, Lawrence E.; Gan, Weiqun; Gizon, Laurent; Heinzl, Petr; Rovira, Marta G.; Venkatakrishnan, P. Bibcode: 2009IAUTA..27..104M Altcode: Commission 12 encompasses investigations on the internal structure and dynamics of the Sun, mostly accessible through the techniques of local and global helioseismology, the quiet solar atmosphere, solar radiation and its variability, and the nature of relatively stable magnetic structures like sunspots, faculae and the magnetic network. A revision of the progress made in these fields is presented. For some specific topics, the review has counted with the help of experts outside the Commission Organizing Committee that are leading and/or have recently presented relevant works in the respective fields. In this cases the contributor's name is given in parenthesis. Title: Flows and Nonthermal Velocities in Solar Active Regions Observed with the EUV Imaging Spectrometer on Hinode: A Tracer of Active Region Sources of Heliospheric Magnetic Fields? Authors: Doschek, G. A.; Warren, H. P.; Mariska, J. T.; Muglach, K.; Culhane, J. L.; Hara, H.; Watanabe, T. Bibcode: 2008ApJ...686.1362D Altcode: 2008arXiv0807.2860D From Doppler velocity maps of active regions constructed from spectra obtained by the EUV Imaging Spectrometer (EIS) on the Hinode spacecraft we observe large areas of outflow (20-50 km s-1) that can persist for at least a day. These outflows occur in areas of active regions that are faint in coronal spectral lines formed at typical quiet-Sun and active region temperatures. The outflows are positively correlated with nonthermal velocities in coronal plasmas. The bulk mass motions and nonthermal velocities are derived from spectral line centroids and line widths, mostly from a strong line of Fe XII at 195.12 Å. The electron temperature of the outflow regions estimated from an Fe XIII to Fe XII line intensity ratio is about (1.2-1.4) × 106 K. The electron density of the outflow regions derived from a density-sensitive intensity ratio of Fe XII lines is rather low for an active region. Most regions average around 7 × 108 cm-3, but there are variations on pixel spatial scales of about a factor of 4. We discuss results in detail for two active regions observed by EIS. Images of active regions in line intensity, line width, and line centroid are obtained by rastering the regions. We also discuss data from the active regions obtained from other orbiting spacecraft that support the conclusions obtained from analysis of the EIS spectra. The locations of the flows in the active regions with respect to the longitudinal photospheric magnetic fields suggest that these regions might be tracers of long loops and/or open magnetic fields that extend into the heliosphere, and thus the flows could possibly contribute significantly to the solar wind. Title: Long Duration Flare Observed with Hinode EIS Authors: Culhane, J. L.; Hara, H.; Watanabe, T.; Matsuzaki, K.; Harra, L. K.; Cargill, P.; Mariska, J. T.; Doschek, G. A. Bibcode: 2008ASPC..397..121C Altcode: The first Long Duration Event (LDE) observed with Hinode EIS using a high spectral resolution raster scan is described. The hot plasma features include a cusp-shaped arcade associated with a thermal RHESSI source, cooling post-flare loops, complex plasma flows and an EIT observation that shows expanding loops and inflows characteristic of the standard magnetic reconnection model for solar flares. A Coronal Mass Ejection (CME) is also seen by LASCO. The cusp is well observed in the Ca XVII line and we find enhanced line broadening above this region. Doppler velocity observations for the post-flare loops show both up-flows and down-flows that are interpreted as due to siphon flows. Title: Doppler Shifts in the Boundary of the Dimming Region Authors: Imada, S.; Hara, H.; Watanabe, T.; Asai, A.; Kamio, S.; Matsuzaki, K.; Harra, L. K.; Mariska, J. T. Bibcode: 2008ASPC..397..102I Altcode: We present Hinode/EIS raster scan observations of the GOES X3.2 flare that occurred on 2006 December 13. There was a small transient coronal hole which was located 200 arcsec east of the flare arcade. The transient coronal hole was strongly affected by the X-class flare, and the strong upflows were observed in Fe XV line 284.2 Å (log{T/{K}} = 6.3) at the boundary of dimming region. In this paper, we discuss how to obtain the velocity map by correcting the instrumental effects. Title: Observations of Doppler Shift Oscillations with the EUV Imaging Spectrometer on Hinode Authors: Mariska, John T.; Warren, Harry P.; Williams, David R.; Watanabe, Tetsuya Bibcode: 2008ApJ...681L..41M Altcode: 2008arXiv0806.0265M Damped Doppler shift oscillations have been observed in emission lines from ions formed at flare temperatures with the Solar Ultraviolet Measurements of Emitted Radiation spectrometer on the Solar and Heliospheric Observatory and with the Bragg Crystal Spectrometer on Yohkoh. This Letter reports the detection of low-amplitude damped oscillations in coronal emission lines formed at much lower temperatures observed with the EUV Imaging Spectrometer on the Hinode satellite. The oscillations have an amplitude of about 2 km s-1 and a period of around 35 minutes. The decay times show some evidence for a temperature dependence with the lowest temperature of formation emission line (Fe XII 195.12 Å) exhibiting a decay time of about 43 minutes, while the highest temperature of formation emission line (Fe XV 284.16 Å) shows no evidence for decay over more than two periods of the oscillation. The data appear to be consistent with slow magnetoacoustic standing waves, but may be inconsistent with conductive damping. Title: Non-Gaussian Line Profiles in a Large Solar Flare Observed on 2006 December 13 Authors: Imada, S.; Hara, H.; Watanabe, T.; Asai, A.; Minoshima, T.; Harra, L. K.; Mariska, J. T. Bibcode: 2008ApJ...679L.155I Altcode: We have studied the characteristics of the non-Gaussian line profile of the Fe XIV 274.20 Å line in and around a flare arcade. We found that broad non-Gaussian line profiles associated with redshifts are observed in the flare arcade. There were two typical types of broad line profiles. One was a distorted line profile caused by multiple flows, and the other was a symmetric line profile without any additional component. We successfully distinguished those two types using higher order statistical moments or M—the additional component contribution—defined in this Letter. The distorted/symmetric broad line profiles were preferentially observed in new/old flare loops, respectively. Title: Observations of Doppler Shift Oscillations With the EUV Imaging Spectrometer on Hinode Authors: Mariska, J. T.; Warren, H. P.; Williams, D. R.; Watanabe, T. Bibcode: 2008AGUSMSP31A..04M Altcode: Damped Doppler shift oscillations have been observed in emission lines from ions formed at flare temperatures with the Solar Ultraviolet Measurements of Emitted Radiation spectrometer on SOHO and the Bragg Crystal Spectrometer on Yohkoh. We report the detection of similar oscillations in coronal emission lines observed with the EUV Imaging Spectrometer on the Hinode satellite. The oscillations, which are present in emission lines formed at lower temperatures than seen with the instruments listed above, have an amplitude of about 2 km s- 1, and a period of around 35 min. The decay times show some evidence for a temperature dependence with the lowest temperature of formation emission line (Fe~XII 195.12 Å) exhibiting a decay time of about 43 min, while the highest temperature of formation emission line (Fe~XV 284.16 Å) shows no evidence for decay over more than two periods of the oscillation. The data appear to be consistent with slow magnetoacoustic standing waves. Title: Coronal Plasma Motions near Footpoints of Active Region Loops Revealed from Spectroscopic Observations with Hinode EIS Authors: Hara, Hirohisa; Watanabe, Tetsuya; Harra, Louise K.; Culhane, J. Leonard; Young, Peter R.; Mariska, John T.; Doschek, George A. Bibcode: 2008ApJ...678L..67H Altcode: The solar active region 10938 has been observed from the disk center to the west limb with the Hinode EUV Imaging Spectrometer. In the disk-center observation, subsonic upflow motions of tens of km s-1 and enhanced nonthermal velocities have been found near the footpoints of the active region loops assuming a single Gaussian approximation for the emission-line profiles. When the same part of the active region is observed near the limb, both upflows and enhanced nonthermal velocities essentially decrease. There is a strong correlation between Doppler velocity and nonthermal velocity. Significant deviations from a single Gaussian profile are found in the blue wing of the line profiles for the upflows. These suggest that there are unresolved high-speed upflows. We discuss the implications for coronal heating mechanisms. Title: Observation and Modeling of Coronal "Moss" With the EUV Imaging Spectrometer on Hinode Authors: Warren, Harry P.; Winebarger, Amy R.; Mariska, John T.; Doschek, George A.; Hara, Hirohisa Bibcode: 2008ApJ...677.1395W Altcode: 2007arXiv0709.0396W Observations of transition region emission in solar active regions represent a powerful tool for determining the properties of hot coronal loops. We present the analysis of new observations of active region moss taken with the Extreme Ultraviolet Imaging Spectrometer (EIS) on the Hinode satellite. EIS observations of a density sensitive Fe XII line ratio suggest moss densities of approximately 1010 cm-3 and pressures of 3 × 1016 cm-3 K. We find that the moss intensities predicted by steady, uniformly heated loop models are too intense relative to the observations, consistent with previous work. To bring the steady heating model into agreement with the observations a filling factor is required. Our analysis indicates that the filling factor in the moss is nonuniform and varies inversely with the loop pressure. The intensities predicted by steady uniform heating are generally consistent with the EIS moss observations. There are, however, significant discrepancies for the coolest emission line available in the data we analyze. Title: 2006 December 17 Long Duration Flare Observed with the Hinode EUV Imaging Spectrometer Authors: Hara, Hirohisa; Watanabe, Tetsuya; Matsuzaki, Keiichi; Harra, Louise K.; Culhane, J. Leonard; Cargill, Peter; Mariska, John T.; Doschek, George A. Bibcode: 2008PASJ...60..275H Altcode: A GOES C-class long-duration flare that occurred near the west limb on 2006 December 17 was observed with the Hinode EUV Imaging Spectrometer (EIS) in raster-scan observations. Cusp-shaped arcades are prominent in the spectroheliogram of the CaXVII emission line at 192.86Å. Spatial relationships between hot flare loops with a cusp apex and cool post flare loops with various temperatures are clearly shown in the EIS observations. We find an enhanced line broadening above the bright loop-top region in the CaXVII observation. The Doppler observations of cooling post flare loops with coronal temperatures show both downflows and upflows along the loops, and these are interpreted as a part of siphon flows. Enhanced nonthermal line broadenings are identified at the top of the post flare loops. Title: Coronal Plasma Motions near Footpoints of Active Region Loops Revealed from Spectroscopic Observations with {it Hinode} EIS Authors: Hara, Hirohisa; Watanabe, Tetsuya; Harra, Louise K.; Culhane, J. Leonard; Young, Peter R.; Doschek, G. A.; Mariska, John Bibcode: 2008cosp...37.1175H Altcode: 2008cosp.meet.1175H We have observed the solar active region 10938 from the disk center to the west limb with the Hinode EUV Imaging Spectrometer. In the disk center observation subsonic upflow motions of tens of km s-1 and enhanced nonthermal velocities have been found near the footpoints of the active-region loops assuming a single Gaussian approximation for the emission-line profiles. When the same part of the active region is observed near the limb, both upflows and enhanced nonthermal velocities essentially decrease, clearly showing that the enhanced nonthermal velocities in the disk center observation are mainly due to line-of-sight motions, which are likely parallel to magnetic field lines of the coronal loops. There is a strong correlation between Doppler velocity and nonthermal velocity in the upflow regions. The enhancement in the blue wing of the line profiles is found for the upflows as a significant deviation from a single Gaussian profile. These suggest that there are unresolved high-speed upflows near the footpoints of active region loops. We discuss the implications for coronal heating mechanisms. Title: The Structure and Dynamics of the Quiet Corona from Observations with the Extreme ultraviolet Imaging Spectrometer Authors: Dere, K. P.; Doschek, G. A.; Mariska, J. T.; Harra, L. K.; Matsuzaki, K.; Hansteen, V.; Thomas, R. J. Bibcode: 2007AGUFMSH53A1046D Altcode: The goal of the Extreme-ultraviolet Imaging Spectrometer (EIS) on the Hinode satellite is to measure such physical parameters as the velocity and density of the solar corona in order to provide an observational basis to understand how coronal plasmas are heated and accelerated. On 2007 January 20, EIS performed a raster of a 128 x 512 arc-sec. area of a quiet region near Sun center. The observing program recorded spectra of He II λ256, formed at 9 × 104 K, and lines of Fe VIII-XV, formed at temperatures spanning the range from 5 × 105 through 2 × 106 K. Maps of intensities, velocities and electron densities derived from these observations are presented and discussed. Intensity maps in He II λ256 show the chromospheric network. Line intensities of Fe X-XIV show small-scale bright points and more extended structures. The intensity map of Fe VIII shows a transition between the two temperatures. The coronal lines reveal regions of high outflow velocities on the order of 100 km s-1 in a compact region and 12 km s-1 in an extended region. The presence of these high velocities in the quiet corona is an entirely new and unexpected result. Electron densities derived from density sensitive line ratios of Fe XII and XIII are typically about 3 - 20×108 cm-3. The highest densities are found in bright, compact areas. For the first time, explosive events in the quiet sun have been observed in the extreme-ultraviolet in He II λ256 profiles and have properties similar to those previously reported. Title: The Structure and Dynamics of the Quiet Corona from Observations with the Extreme Ultraviolet Imaging Spectrometer on Hinode Authors: Dere, Kenneth P.; Doschek, George A.; Mariska, John T.; Hansteen, Viggo H.; Harra, Louise K.; Matsuzaki, Keiichi; Thomas, Roger J. Bibcode: 2007PASJ...59S.721D Altcode: The goal of the Hinode mission is to provide an observational basis for understanding the heating and acceleration of coronal plasmas. On 2007 January 20, the Extreme ultraviolet Imaging Spectrometer performed a raster of a quiet region near Sun center. Maps of intensities, velocities, and electron densities derived from these observations are presented and discussed. Intensity maps in HeII λ 256, formed at 9 × 104 K, show the chromospheric network. Line intensities of FeX-XIV, formed at temperatures from 1-2 × 106 K, show small-scale bright points and more extended structures. The intensity map of FeVIII shows a transition between the two temperatures. The coronal lines reveal regions of high outflow velocities on the order of 100kms-1 in a compact region and 12kms-1 in an extended region. The presence of such high velocities in the quiet corona is an entirely new and unexpected result. Electron densities derived from density sensitive line ratios of FeXII and XIII are typically 3-20 × 108cm-3. The highest densities are found in bright, compact areas. For the first time, explosive events in the quiet sun have been observed in the extreme-ultraviolet in HeII λ 256 profiles. Title: Temperature and Density Structures of Solar Corona, A Test of Iron Line Diagnostic Capability of EIS Instrument on Board Hinode Authors: Watanabe, Tetsuya; Hara, Hirohisa; Culhane, Len; Harra, Louise K.; Doschek, George A.; Mariska, John T.; Young, Peter R. Bibcode: 2007PASJ...59S.669W Altcode: Increased diagnostic capability of the EUV Imaging Spectrometer (EIS) aboard Hinode (former Solar-B) has been demonstrated with a set of iron emission lines emerging in the two EIS observing wavelength bands (170-210Å and 250-290Å) and their line-intensity ratios. ``Abundance-uncertainty'' free relative emission measure distributions as a function of temperature were deduced using only iron emission lines of various ionization stages. First-light spectra of a small active region show iron lines ranging from FeVIII (185.2Å and 186.6Å) through FeXVII (204.7Å, 254.9Å, and 269.4Å). Spectra of a C-class flare confirms the presence of one of these higher temperature lines (FeXVII at 254.9Å) more clearly, as well showing FeXXIV (192.0Å and 255.1Å) and FeXXIII (263.8Å), which are normally only seen at flare temperatures. Title: The Temperature and Density Structure of an Active Region Observed with the Extreme-Ultraviolet Imaging Spectrometer on Hinode Authors: Doschek, George A.; Mariska, John T.; Warren, Harry P.; Culhane, Len; Watanabe, Tetsuya; Young, Peter R.; Mason, Helen E.; Dere, Kenneth P. Bibcode: 2007PASJ...59S.707D Altcode: The Extreme-Ultraviolet Imaging Spectrometer (EIS) on Hinode produces high resolution spectra that can be combined via rasters into monochromatic images of solar structures, such as active regions. Electron temperature and density maps of the structures can be obtained by imaging the structures in different spectral lines with ratios sensitive to either temperature or density. Doppler maps and ion temperature maps can be made from spectral line wavelengths and profiles, respectively. In this paper we discuss coronal temperature and density distributions within an active region, illustrating the power of EIS for solar plasma diagnostics. Title: Hinode EUV Imaging Spectrometer Observations of Solar Active Region Dynamics Authors: Mariska, John T.; Warren, Harry P.; Ugarte-Urra, Ignacio; Brooks, David H.; Williams, David R.; Hara, Hirohisa Bibcode: 2007PASJ...59S.713M Altcode: 2007arXiv0708.4309M The EUV Imaging Spectrometer (EIS) on the Hinode satellite is capable of measuring emission line center positions for Gaussian line profiles to a fraction of a spectral pixel, resulting in relative solar Doppler-shift measurements with an accuracy of a less than a km s-1 for strong lines. We show an example of the application of that capability to an active region sit-and-stare observation in which the EIS slit is placed at one location on the Sun and many exposures are taken while the spacecraft tracking keeps the same solar location within the slit. For the active region examined (NOAA10930), we find that significant intensity and Doppler-shift fluctuations as a function of time are present at a number of locations. These fluctuations appear to be similar to those observed in high-temperature emission lines with other space-borne spectroscopic instruments. With its increased sensitivity over earlier spectrometers and its ability to image many emission lines simultaneously, EIS should provide significant new constraints on Doppler-shift oscillations in the corona. Title: Discovery of a Temperature-Dependent Upflow in the Plage Region During a Gradual Phase of the X-Class Flare Authors: Imada, Shinsuke; Hara, Hirohisa; Watanabe, Tetsuya; Kamio, Suguru; Asai, Ayumi; Matsuzaki, Keiichi; Harra, Louise K.; Mariska, John T. Bibcode: 2007PASJ...59S.793I Altcode: We present Hinode/EIS raster scan observations of the plage region taken during the gradual phase of the GOES X3.2 flare that occurred on 2006 December 13. The plage region is located 200" east of the flare arcade. The plage region has a small transient coronal hole. The transient coronal hole is strongly affected by an X-class flare, and upflows are observed at its boundary. Multi-wavelength spectral observations allow us to determine velocities from the Doppler shifts at different temperatures. Strong upflows along with stationary plasma have been observed in the FeXV line 284.2Å (log T / K = 6.3) in the plage region. The strong upflows reach almost 150kms-1, which was estimated by a two-component Gaussian fitting. On the other hand, at a lower corona/transition region temperature (HeII, 256.3Å, log T / K = 4.9), very weak upflows, almost stationary, have been observed. We find that these upflow velocities clearly depend on the temperature with the hottest line, FeXV, showing the fastest upflow velocity and the second-highest line, FeXIV, showing the second-highest upflow velocity (130kms-1). All velocities are below the sound speed. The trend of the upflow dependence on temperature dramatically changes at 1MK. These results suggest that heating may have an important role for strong upflow. Title: Wavelength Determination for Solar Features Observed by the EUV Imaging Spectrometer on Hinode Authors: Brown, Charles M.; Hara, Hirohisa; Kamio, Suguru; Feldman, Uri; Seely, John F.; Doschek, George A.; Mariska, John T.; Korendyke, Clarence M.; Lang, James; Dere, Kenneth P.; Culhane, Len; Thomas, Roger J.; Davila, Joseph M. Bibcode: 2007PASJ...59S.865B Altcode: A wavelength calibration of solar lines observed by the high resolution EUV Imaging Spectrometer (EIS) on the Hinode satellite is reported. Spectral features of the quiet sun and of two mildly active areas were measured and calibrated. A listing of the stronger observed lines with identification of the leading contributor ions is presented. 41 lines are reported, with 90% identified. Wavelength precisions (2σ) of ±0.0031Å for the EIS short band and ±0.0029Å for the EIS long band are obtained. These lines, typical of 1-2 ×106 K plasmas, are recommended as standards for the establishment of EIS wavelength scales. The temperature of EIS varies by about 1D.5 C around the orbit and also with spacecraft pointing. The correlation of these temperature changes with wavelength versus pixel number scale changes is reported. Title: Nonthermal Velocities in Solar Active Regions Observed with the Extreme-Ultraviolet Imaging Spectrometer on Hinode Authors: Doschek, G. A.; Mariska, J. T.; Warren, H. P.; Brown, C. M.; Culhane, J. L.; Hara, H.; Watanabe, T.; Young, P. R.; Mason, H. E. Bibcode: 2007ApJ...667L.109D Altcode: We discuss nonthermal velocities in an active region as revealed by the Extreme-Ultraviolet Imaging Spectrometer (EIS) on the Hinode spacecraft. The velocities are derived from spectral line profiles in the extreme-ultraviolet (EUV) from a strong line of Fe XII at 195.12 Å by fitting each line profile to a Gaussian function. We compare maps of the full width at half-maximum values, the Fe XII spectral line intensity, the Fe XII Doppler shift, the electron temperature, and electron density. We find that the largest widths in the active region do not occur in the most intense regions, but seem to concentrate in less intense regions, some of which are directly adjacent to coronal loops, and some of which concentrate in regions which also exhibit relative Doppler outflows. The increased widths can also occur over extended parts of the active region. Title: The EUV Imaging Spectrometer for Hinode Authors: Culhane, J. L.; Harra, L. K.; James, A. M.; Al-Janabi, K.; Bradley, L. J.; Chaudry, R. A.; Rees, K.; Tandy, J. A.; Thomas, P.; Whillock, M. C. R.; Winter, B.; Doschek, G. A.; Korendyke, C. M.; Brown, C. M.; Myers, S.; Mariska, J.; Seely, J.; Lang, J.; Kent, B. J.; Shaughnessy, B. M.; Young, P. R.; Simnett, G. M.; Castelli, C. M.; Mahmoud, S.; Mapson-Menard, H.; Probyn, B. J.; Thomas, R. J.; Davila, J.; Dere, K.; Windt, D.; Shea, J.; Hagood, R.; Moye, R.; Hara, H.; Watanabe, T.; Matsuzaki, K.; Kosugi, T.; Hansteen, V.; Wikstol, Ø. Bibcode: 2007SoPh..243...19C Altcode: The EUV Imaging Spectrometer (EIS) on Hinode will observe solar corona and upper transition region emission lines in the wavelength ranges 170 - 210 Å and 250 - 290 Å. The line centroid positions and profile widths will allow plasma velocities and turbulent or non-thermal line broadenings to be measured. We will derive local plasma temperatures and densities from the line intensities. The spectra will allow accurate determination of differential emission measure and element abundances within a variety of corona and transition region structures. These powerful spectroscopic diagnostics will allow identification and characterization of magnetic reconnection and wave propagation processes in the upper solar atmosphere. We will also directly study the detailed evolution and heating of coronal loops. The EIS instrument incorporates a unique two element, normal incidence design. The optics are coated with optimized multilayer coatings. We have selected highly efficient, backside-illuminated, thinned CCDs. These design features result in an instrument that has significantly greater effective area than previous orbiting EUV spectrographs with typical active region 2 - 5 s exposure times in the brightest lines. EIS can scan a field of 6×8.5 arc min with spatial and velocity scales of 1 arc sec and 25 km s−1 per pixel. The instrument design, its absolute calibration, and performance are described in detail in this paper. EIS will be used along with the Solar Optical Telescope (SOT) and the X-ray Telescope (XRT) for a wide range of studies of the solar atmosphere. Title: A Long-duration Flare Observed With Hinode EIS Authors: Hara, Hirohisa; Watanabe, T.; Harra, L.; Culhane, L.; Cargill, P.; Doschek, G.; Mariska, J. Bibcode: 2007AAS...210.6802H Altcode: 2007BAAS...39..175H Long-duration solar flares generally have a cusp apex at the loop top. The cusp shape reflects the topology of magnetic fields near the flare-loop top and it is one of the indirect pieces of evidence supporting the occurrence of the magnetic reconnection process above flare loops. The Hinode EUV Imaging Spectrometer (EIS) observed a long-duration flare that occurred on 2006 Dec 17. We present the first EIS spectroscopic observation of cusp-shaped flare loops. We also report velocity fields around the cusp structures and post-flare loops. Title: Hinode EIS Observations of Solar Active Regions Authors: Mariska, John T.; Doschek, G. A.; Warren, H. P.; Brooks, D. H.; Young, P. R.; Watanabe, T.; Culhane, J. L. Bibcode: 2007AAS...210.7202M Altcode: 2007BAAS...39R.178M The EUV Imaging Spectrometer (EIS) on the Hinode satellite provides high spatial and spectral resolution data along a 512 arcsec slit in two wavelength ranges, 170--210 Angstroms and 250--290 Angstroms. These wavelengths mostly contain emission lines from upper transition region and coronal plasmas. Emission from these wavelengths is routinely imaged using instruments such as the EIT on SOHO and TRACE, but there are few high-resolution spectra to aid in more deeply understanding the physical conditions and dynamics associated with the intensity variations seen in the images. In this presentation, we show some initial results from EIS active region studies aimed at mapping the density, temperature, nonthermal broadening, and Doppler shifts in active regions. This presentation focusses on spectroheliograms of active regions in diagnostically interesting spectral lines. These show the overall active region morphology and the behavior of Doppler shifts, nonthermal velocities, and densities as a function of position, but at the expense of high time resolution. Other presentations will focus on how the observed physical parameters vary with time. Title: Iron Line Ratio Analysis in an Active Region Authors: Watanabe, Tetsuya; Hara, H.; Culhane, J. L.; Harra, L. K.; Doschek, G. A.; Mariska, J. T.; Young, P. R.; Hinode EIS Team Bibcode: 2007AAS...210.7204W Altcode: 2007BAAS...39..179W Increased diagnostic capability of the EIS instrument on board Hinode (Solar-B) is demonstrated with a set of iron emission lines appearing in the two EIS observing wavelengths (170 - 210 A & 250 - 290 A) and their line intensity ratios. First-light spectra of a small active region show iron lines at the ionization stages of FeVIII (185.2 A & 186.6 A) through FeXVII (204.7 A, 254.9 A, & 269.4 A). Decay phase spectra of a C-class flare confirms the presence of this higher temperature line; FeXVII at 254.9 A more clearly, as well as those lines of flare temperatures; FeXXIV (192.0 A & 255.1 A) and FeXXIII (263.8 A). Title: Commission 12: Solar Radiation & Structure Authors: Bogdan, Thomas. J.; Martínez Pillet, Valentin; Asplund, M.; Christensen-Dalsgaard, J.; Cauzzi, G.; Cram, L. E.; Dravins, D.; Gan, W.; Henzl, P.; Kosovichev, A.; Mariska, J. T.; Rovira, M. G.; Venkatakrishnan, P. Bibcode: 2007IAUTA..26...89B Altcode: Commission 12 covers research on the internal structure and dynamics of the Sun, the "quiet" solar atmosphere, solar radiation and its variability, and the nature of relatively stable magnetic structures like sunspots, faculae and the magnetic network. There is considerable productive overlap with the other Commissions of Division II as investigations move progressively toward the fertile intellectual boundaries between traditional research disciplines. In large part, the solar magnetic field provides the linkage that connects these diverse themes. The same magnetic field that produces the more subtle variations of solar structure and radiative output over the 11 yr activity cycle is also implicated in rapid and often violent phenomena such as flares, coronal mass ejections, prominence eruptions, and episodes of sporadic magnetic reconnection.The last three years have again brought significant progress in nearly all the research endeavors touched upon by the interests of Commission 12. The underlying causes for this success remain the same: sustained advances in computing capabilities coupled with diverse observations with increasing levels of spatial, temporal and spectral resolution. It is all but impossible to deal with these many advances here in anything except a cursory and selective fashion. Thankfully, the Living Reviews in Solar Physics; has published several extensive reviews over the last two years that deal explicitly with issues relevant to the purview of Commission 12. The reader who is eager for a deeper and more complete understanding of some of these advances is directed to http://www.livingreviews.org for access to these articles. Title: Optics and mechanisms for the Extreme-Ultraviolet Imaging Spectrometer on the Solar-B satellite Authors: Korendyke, Clarence M.; Brown, Charles M.; Thomas, Roger J.; Keyser, Christian; Davila, Joseph; Hagood, Robert; Hara, Hirohisa; Heidemann, Klaus; James, Adrian M.; Lang, James; Mariska, John T.; Moser, John; Moye, Robert; Myers, Steven; Probyn, Brian J.; Seely, John F.; Shea, John; Shepler, Ed; Tandy, Jason Bibcode: 2006ApOpt..45.8674K Altcode: The Extreme-Ultraviolet Imaging Spectrometer (EIS) is the first of a new generation of normal-incidence, two-optical-element spectroscopic instruments developed for space solar extreme-ultraviolet astronomy. The instrument is currently mounted on the Solar-B satellite for a planned launch in late 2006. The instrument observes in two spectral bands, 170-210 Å and 250-290 Å. The spectrograph geometry and grating prescription were optimized to obtain excellent imaging while still maintaining readily achievable physical and fabrication tolerances. A refined technique using low ruling density surrogate gratings and optical metrology was developed to align the instrument with visible light. Slit rasters of the solar surface are obtained by mechanically tilting the mirror. A slit exchange mechanism allows selection among four slits at the telescope focal plane. Each slit is precisely located at the focal plane. The spectrograph imaging performance was optically characterized in the laboratory. The resolution was measured using the Mg iii and Ne iii lines in the range of 171-200 Å. The He ii line at 256 Å and Ne iii lines were used in the range of 251-284 Å. The measurements demonstrate an equivalent resolution of ∼2 arc sec⁡ on the solar surface, in good agreement with the predicted performance. We describe the EIS optics, mechanisms, and measured performance. Title: The extreme UV imaging spectrometer for the JAXA Solar-B mission Authors: Culhane, J. L.; Doschek, G. A.; Watanabe, T.; Smith, A.; Brown, C.; Hara, H.; Harra, L. K.; James, A. M.; al Janabi, K.; Kent, B.; Korendyke, C.; Lang, J.; Mariska, J.; Myers, S.; Seely, J.; Simnett, G.; Tandy, J.; Thomas, R.; Windt, D. L. Bibcode: 2006SPIE.6266E..0TC Altcode: 2006SPIE.6266E..22C The ISAS/JAXA Solar-B mission includes an Extreme-UV Imaging Spectrometer (EIS). It detects photons in the wavelength ranges 17 - 21 nm and 25 - 29 nm which include emission lines from several highly ionised species that exist at temperatures log T = 4.7, 5.6, 5.8, 5.9 and 6.0 - 7.3 K. Instrument throughput is increased substantially by the use of multilayer coatings optimized for maximum reflectance in the two selected wavelength bands. The use of back-illuminated CCDs provides significantly enhanced quantum efficiency over that previously available from microchannel plate systems. In this paper we will describe the design and operation of the instrument and present its performance parameters e.g. spectral and spatial resolution and sensitivity. Preliminary results of recent calibration measurements will be described. The role of EIS in the Solar-B mission will be illustrated with reference to the anticipated observing strategy for the first three months of the mission which will be outlined. Title: X-ray Emission from Flaring Loops: Comparison Between RHESSI Observations and Hydrodynamic Simulations Authors: Liu, Wei; Jiang, Y. W.; Petrosian, V.; Liu, S.; Mariska, J. T. Bibcode: 2006SPD....37.2705L Altcode: 2006BAAS...38..254L RHESSI with its high temporal, spatial, and spectral resolution has revealed many interesting results on the X-ray emission from solar flares, some of which can shed light on the processes of energy release, particle acceleration, heating, and evaporation of chromospheric plasmas. During the impulsive phase of a limb flare, Liu et al. (2006) reported hard X-ray (HXR) emission dominated by the legs of the loop, as opposed to the commonly observed loop top (LT) and footpoint (FP) emissions. The HXR emission tends to rise above the FPs and eventually merge into a single LT source, suggestive of a gradual density increase in the loop possibly caused by chromospheric evaporation. During the decay phase of six limb flares, Jiang et al. (2006) found that the thermal LT source is confined in a small region near the top of the loop rather than spreading throughout the whole loop. The total energy of the source decays much slower than expected from the classical Spitzer conductive cooling alone. A quasi-steady loop model that includes significant suppression of thermal conductivity and/or continuous heating of the LT plasma, presumably by plasma wave turbulence, was proposed to account for this observation. A more thorough understanding of these phenomena requires a solution of the time-dependent hydrodynamics of the flaring plasma. We have embarked on combining our particle acceleration and transport code with a one-dimensional hydrodynamics code (Mariska et al. 1989) to simulate the response of the atmosphere to the energy input during the impulsive and decay phases, and investigate the effects of such response on the energy transport, X-ray radiation, and even particle acceleration and plasma heating processes. Current results from this work in progress will be presented. We will also compare the results with RHESSI observations and thus put important constraints on theoretical models. Title: The Extreme Ultraviolet Imaging Spectrometer (EIS) on Solar-B Authors: Doschek, George A.; Brown, C. M.; Korendyke, C. M.; Mariska, J. T.; Myers, S. H.; Seely, J. F.; Dere, K. P.; Lang, J.; Culhane, J. L.; Watanabe, T. Bibcode: 2006SPD....37.3604D Altcode: 2006BAAS...38S.260D The Extreme Ultraviolet Imaging Spectrometer (EIS) for Solar-B is a high throughput state-of-the-art instrument designed to obtain solar spectra and images in two wavelength bands centered near 195 and 270 Angstroms. Traditional spectra can be obtained using narrow slits or images of solar structures can be obtained in individual spectral lines using wide slots. Essentially, the instrument obtains images in wavebands similar to TRACE but in each spectral line within the waveband. This removes electron temperature ambiguities inherent in broadband imagers and allows dynamic effects to be detected via Doppler shifts and densities and other plasma parameters to be measured via spectroscopic plasma diagnostics. After a brief description of how the instrument works and a comparison with previous instrumentation (sensitivity, etc.), the presentation will focus on the science that can be accomplished with EIS, presented in the form of sample observing sequences. The focus will be on active regions and solar flares with a consideration of topics such as temperature and density distributions in active region loops and their evolution, dynamical motions in active region loops, the reconnection site in solar flares, and temperature evolution of multimillion degree flare loops. Title: Observations and Modeling of Solar Flare Doppler-Shift and Intensity Oscillations Authors: Mariska, John T. Bibcode: 2006SPD....37.1307M Altcode: 2006BAAS...38..241M Doppler-shift and associated intensity oscillations have been observed in high-temperature flare emission lines with both the SUMER experiment on SOHO and the Bragg Crystal Spectrometer (BCS) on Yohkoh. These have been identified as standing slow-mode waves, leading to the possibility that modeling of the wave evolution can lead to improved understanding of the conditions in the flaring structures. In this presentation, I show some examples of the BCS data and initial results from loop heating numerical simulations aimed at studying the initiation and evolution of the oscillations. Many impulsive heating schemes easily excite oscillations in the loop plasma. A key issue for investigation, however, is whether detailed geometric information on the flaring loop or loops coupled with the oscillation observations can critically constrain the characteristics of the heating. Title: Characteristics of Solar Flare Doppler-Shift Oscillations Observed with the Bragg Crystal Spectrometer on Yohkoh Authors: Mariska, John T. Bibcode: 2006ApJ...639..484M Altcode: 2005astro.ph.11070M This paper reports the results of a survey of Doppler-shift oscillations measured during solar flares in emission lines of S XV and Ca XIX with the Bragg Crystal Spectrometer (BCS) on Yohkoh. Data from 20 flares that show oscillatory behavior in the measured Doppler shifts have been fitted to determine the properties of the oscillations. Results from both BCS channels show average oscillation periods of 5.5+/-2.7 minutes, decay times of 5.0+/-2.5 minutes, amplitudes of 17.1+/-17.0 km s-1, and inferred displacements of 1070+/-1710 km, where the listed errors are the standard deviations of the sample means. For some of the flares, intensity fluctuations are also observed. These lag the Doppler-shift oscillations by 1/4 period, strongly suggesting that the oscillations are standing slow-mode waves. The relationship between the oscillation period and the decay time is consistent with conductive damping of the oscillations. Title: Observing the Solar atmosphere with the Extreme Ultraviolet Imaging Spectrometer on Solar B Authors: Korendyke, C. M.; Brown, C.; Dere, K.; Doschek, G.; Klimchuk, J.; Landi, E.; Mariska, J.; Warren, H.; Lang, J. Bibcode: 2005AGUFMSH41B1124K Altcode: The Extreme Ultraviolet Imaging Spectrometer (EIS) is part of the instrument complement on the Solar B satellite, scheduled for launch in the summer of 2006. The instrument has been calibrated and is presently mounted on the spacecraft. EIS is the most sensitive EUV solar spectrometer to be flown. The instrument is the first of a new generation of two optical element, solar spectrographs. Preliminary results from the laboratory focussing and calibration of the instrument will be shown. The instrument wavelength coverage includes reasonably bright spectral lines emitted by plasmas from 0.1 to 20 MK in temperature. The wavelength range also provides coronal density diagnostics. Temperature, density and velocity diagnostics will be discussed. An example observing program for exploring active region evolution and dynamics will be discussed. Title: A new method for in-flight intensity calibration of high-resolution EUV and FUV spectrometers Authors: Feldman, U.; Landi, E.; Doschek, G. A.; Mariska, J. T. Bibcode: 2005A&A...441.1211F Altcode: We introduce a new technique for the measurement of the in-flight relative intensity calibration of high resolution spectrometers. This technique makes use of the free-free radiation in hot, dense active regions and flares, and combines it with spectral line intensities in an iterative procedure. After a few iterations, the relative intensity calibration and the temperature of the emitting plasma are determined. The application of this technique to the EIS instrument on board the Solar-B satellite (launch in 2006) is discussed. Title: The Extreme Ultraviolet Imaging Spectrometer on Solar-B Authors: Mariska, J. T.; Brown, C. M.; Doschek, G. A.; Korendyke, C. M.; Myers, S. H.; Seely, J. F.; Dere, K. P.; Lang, J.; Culhane, J. L.; Watanabe, T. Bibcode: 2005AGUSMSP43A..02M Altcode: The Extreme Ultraviolet Imaging Spectrometer (EIS) is currently under development for flight on the Japanese Solar-B satellite. EIS uses a multilayer-coated off-axis telescope mirror and a multilayer-coated toroidal grating spectrometer to produce stigmatic spectra of solar regions isolated by a 1024 arcsec high slit. The instrument produces monochromatic images either by rastering the solar image across a narrow entrance slit or by using a very wide slit. Half of each optic is coated to optimize reflectance at 19.5 nm, and the other half to optimize reflectance at 27.0 nm, with each wavelength range imaged onto a separate CCD detector. EIS can provide key dynamical and density diagnostic information. Combining EIS data with observations from the other instruments on Solar-B should provide a detailed picture of solar atmospheric processes from the visible surface into the corona. In this presentation, we provide details of the instrument's expected performance based on calibration of the individual flight optics and end-to-end testing at the Rutherford Appleton Laboratory in the UK. Title: Stochastic Particle Acceleration in a Self-Consistent Solar Flare Atmosphere Authors: Miller, J. A.; Mariska, J. T. Bibcode: 2005AGUSMSP41C..02M Altcode: We present results from a unified and self-consistent model of particle acceleration and atmospheric response in impulsive solar flares. In our model, electrons and ions are stochastically energized from thermal to relativistic energies on short timescales by cascading MHD turbulence, which is assumed to have been excited initially in the coronal region of a flare loop during the primary energy release phase. The accelerated particles then propagate to the denser transition region and chromosphere, where they can deposit a large fraction of their energy and drive the formation of a hydrodynamic shock that propagates back into the corona. The density enhancements that accompany this shock in turn modify the particle acceleration processes in the corona by altering (in a spatially-dependent manner) the density and Alfvén speed, and hence the acceleration rates and threshold energies. The two main components of this simulation are the NRL Dynamic Solar Flux Tube Model code and a spatially-dependent quasilinear particle acceleration/wave evolution code. As such, it provides a comprehensive treatment of both macroscopic (chromospheric evaporation) and microscopic (wave-particle interactions) processes. We demonstrate the coupling between acceleration and atmospheric response by presenting simulation results for realistic flare parameters, and show the importance of including the later process in particle acceleration studies. We also show that acceleration by cascading MHD turbulence is able to account for all the major features of flare energetic particles. This work was supported by NASA grant NAG5-12794. Title: Nonthermal Velocities in Different Temperature Regions of the Solar Lower Transition Region Authors: Akiyama, S.; Doschek, G. A.; Mariska, J. T. Bibcode: 2005ApJ...623..540A Altcode: We analyze the relationship between nonthermal velocities derived from spectral lines of ions formed at different temperatures in the solar lower transition region, using spectra from the Solar Ultraviolet Measurements of Emitted Radiation (SUMER) spectrometer on board the Solar and Heliospheric Observatory (SOHO). We find a high degree of correlation among nonthermal motions arising at temperatures ranging from 3×104 to 2.5×105 K over 1" spatial scales in quiet-Sun regions. We discuss the implications of these results in terms of the physical nature of the transition region. Title: Observations of Solar Flare Doppler Shift Oscillations with the Bragg Crystal Spectrometer on Yohkoh Authors: Mariska, John T. Bibcode: 2005ApJ...620L..67M Altcode: 2005astro.ph..1093M Oscillations in solar coronal loops appear to be a common phenomenon. Transverse and longitudinal oscillations have been observed with both the Transition Region and Coronal Explorer and Extreme ultraviolet Imaging Telescope imaging experiments. Damped Doppler shift oscillations have been observed in emission lines from ions formed at flare temperatures with the Solar Ultraviolet Measurements of Emitted Radiation spectrometer. These observations provide valuable diagnostic information on coronal conditions and may help refine our understanding of coronal heating mechanisms. I have initiated a study of the time dependence of Doppler shifts measured during flares with the Bragg Crystal Spectrometer (BCS) on Yohkoh. This Letter reports the detection of oscillatory behavior in Doppler shifts measured as a function of time in the emission lines of S XV and Ca XIX. For some flares, both lines exhibit damped Doppler shift oscillations with amplitudes of a few kilometers per second and periods and decay times of a few minutes. The observations appear to be consistent with transverse oscillations. Because the BCS observed continuously for almost an entire solar cycle, it provides numerous flare data sets, which should permit an excellent characterization of the average properties of the oscillations. Title: The Solar-B EUV imaging spectrometer and its science goals Authors: Culhane, J. L.; Harra, L. K.; Doschek, G. A.; Mariska, J. T.; Watanabe, T.; Hara, H. Bibcode: 2005AdSpR..36.1494C Altcode: The Solar-B mission includes an Extreme-UV Imaging Spectrometer (EIS). It detects photons in the ranges 170-210 and 250-290 Å which include emission lines from several highly ionised species that exist at temperatures log T = 4.7, 5.6, 5.8, 5.9 and 6.0-7.3 K. In this paper, we will describe the design and operation of the instrument and present its performance parameters, e.g., spectral and spatial resolution and sensitivity. Preliminary results of recent calibration measurements will be described. Its role in the Solar-B mission will be illustrated with reference to several key science topics that the EIS is expected to address. The anticipated observing strategy for the first three months of the mission will be outlined. Title: A Unified Model of Particle Acceleration and Atmospheric Response in Solar Flares Authors: Miller, J. A.; Mariska, J. T. Bibcode: 2004AGUFMSH13A1149M Altcode: We present initial results from a unified and self-consistent model of particle acceleration and atmospheric response in impulsive solar flares. In our model, electrons and ions are stochastically energized from thermal to relativistic energies on short timescales by cascading MHD turbulence, which is assumed to have been excited initially in the coronal region of a flare loop during the primary energy release phase. The accelerated particles then propagate to the denser transition region and chromosphere, where they can deposit a large fraction of their energy and drive the formation of a hydrodynamic shock that propagates back into the corona. The density enhancements that accompany this shock in turn modify the particle acceleration process in the corona. The two main components of the simulation are the NRL Dynamic Solar Flux Tube Model code and a spatially-dependent quasilinear particle acceleration/wave evolution code. We demonstrate through these realistic simulations that stochastic acceleration by MHD turbulence is able to account for all the major features of solar flare energetic particles. This work was supported by NASA grant NAG5-12794. Title: The Relationship of the Chromosphere to the Lower Solar Transition Region Authors: Doschek, G. A.; Mariska, J. T.; Akiyama, S. Bibcode: 2004ApJ...609.1153D Altcode: We examine the intensity correlations among lower transition region emission lines of N III, N IV, N V, O II, O III, O IV, O V, S IV, and S V. We find strong intensity correlations, with 1 σ deviations in line intensity ratios less than about 35% on spatial scales of 1". For strong lines the percent deviations are significantly less than this. The line intensities were obtained from the Solar Ultraviolet Measurement of Emitted Radiation (SUMER) spectrometer on the Solar and Heliospheric Observatory (SOHO). We find a dependence of the O II/O III and O V/N V ratios with intensity. The degree of correlation we obtain on arcsecond spatial scales is consistent with size scales for the basic transition region structures that are significantly less than 1" (730 km). Title: Observations of Doppler Shift Oscillations with the Bragg Crystal Spectrometer on Yohkoh Authors: Mariska, J. T. Bibcode: 2004AAS...204.5410M Altcode: 2004BAAS...36..759M Oscillations in solar coronal loops appear to be a common phenomenon. Transverse and longitudinal oscillations have been observed with both the TRACE and EIT imaging experiments. Damped Doppler shift oscillations have been observed in emission lines from ions formed at flare temperatures with the SUMER experiment on SOHO. These observations provide valuable diagnostic information on coronal conditions and may help refine our understanding of coronal heating mechanisms. We have initiated a study of the time dependence of Doppler shifts measured during flares with the Bragg Crystal Spectrometer on Yohkoh. In this presentation, we report some initial results on Doppler shifts as a function of time measured in the emission lines of \ion{S}{15} and \ion{Ca}{19}. For some flares, both lines exhibit damped Doppler shift oscillations with amplitudes of a few km s-1 and periods and decay times of a few minutes. Title: Performance of multilayer-coated gratings for the extreme-ultraviolet imaging spectrometer (EIS) for the Solar-B mission Authors: Seely, John F.; Windt, David L.; Donguy, Soizik; Brown, Charles; Holland, Glenn; Hunter, William R.; Kowalski, Michael P.; Kjornrattanawanich, Benjawan; Doschek, George; Mariska, John; Korendyke, Clarence; Dere, Ken Bibcode: 2004SPIE.5168...12S Altcode: The measured efficiencies of two flight gratings and the reflectances of two flight mirrors developed for the Extreme-Ultraviolet Imaging Spectrometer (EIS) for the Japanese Solar-B mission are presented. Each optic has two sectors with Mo/Si multilayers that refelct the 17 - 21 nm and 25 - 29 nm wavebands at normal incidence. The efficiencies that were measured using monochromatic synchrotron radiation are in good agreement with the calculated efficiencies. Title: Solar Extreme Ultraviolet and X-ray Irradiance Variations Authors: Woods, Tom; Acton, Loren W.; Bailey, Scott; Eparvier, Frank; Garcia, Howard; Judge, Darrell; Lean, Judith; Mariska, John T.; McMullin, Don; Schmidtke, Gerhard; Solomon, Stanley C.; Tobiska, W. Kent; Warren, Harry P.; Viereck, Rodney Bibcode: 2004GMS...141..127W Altcode: The solar extreme ultraviolet (EUV) radiation at wavelengths shortward of 120 nm is a primary energy source for planetary atmospheres and is also a tool for remote sensing of the planets. For such aeronomic studies, accurate values of the solar EUV irradiance are needed over time periods of minutes to decades. There has been a variety of solar EUV irradiance measurements since the 1960s, but most of the recent observations have been broadband measurements in the X-ray ultraviolet (XUV) at wavelengths shortward of 35 nm. A summary of the solar EUV irradiance measurements and their variability during the last decade is presented. One of the most significant new solar irradiance results is the possibility that the irradiance below 20 nm is as much as a factor of 4 higher than the reference Atmospheric Explorer E (AE-E) spectra established in the 1970s and 1980s. The primary short-term irradiance variability is caused by the solar rotation, which has a mean period of 27 days. The primary long-term variability is related to the solar dynamo and is known best by the 11-year sunspot cycle. The solar cycle variability as a function of wavelength can be characterized as 20% to 70% between 120 and 65 nm and as a factor of 1.5 to 10 between 65 and 1 nm. The variability of the total solar EUV irradiance, integrated from 0 to 120 nm, is estimated to be 30-40% for a large 27-day rotational period and a factor of about 2 for the 11-year solar cycle during the recent, rather active, solar cycles. Title: NRLEUV 2: A New Model of Solar EUV Irradiance Variability Authors: Warren, H.; Mariska, J. Bibcode: 2004cosp...35.1109W Altcode: 2004cosp.meet.1109W NRLEUV represents an independent approach to modeling the Sun's EUV irradiance and its variability. Our model utilizes differential emission measure distributions derived from spatially and spectrally resolved solar observations, full-disk solar images, and an a database of atomic physics parameters to calculate the solar EUV irradiance. Our initial version of the model made use of Skylab spectra and a crude partitioning of solar features into quiet Sun, coronal hole, and active region components. Despite the simplicity of our initial effort, our model was able to reproduce the observed EUV irradiance variability at many wavelengths as well as most existing models based directly on observations. In this presentation we will discuss a revised version of the model that is based on extensive observations with the spectrometers on SOHO, utilizes a continuous distribution of emission measures, and includes the most comprehensive database of atomic physics parameters available. Comparisons between our model, other empirical irradiance models, and recent irradiance observations will also be discussed. Title: The spatial correlation of the non-thermal velocities for O IV and Si IV in the lower transition region Authors: Akiyama, S.; Doschek, G. A.; Mariska, J. T. Bibcode: 2003AdSpR..32.1137A Altcode: We analyze the spatial relationship between non-thermal velocities derived from spectral lines of O IV. λ1401.16 (1.6×105 K) and Si IV λ1402.77 (6.3x10 4 K) in the solar lower transition region. The lines formed at different temperatures are observed simultaneously and at the same locations on the solar disk by the Solar Ultraviolet Measurements of Emitted Radiation (SUMER) spectrometer on board the Solar and Heliospheric Observatory (S OHO). In order to improve the accuracy of the non-thermal velocities determined from the full width at half maximum (FVJHM) intensities of the lines, we select data with sufficient counting statistics such that the uncertainty of the non-thermal velocity is less than 10 % of its value derived from the FWHMs. The spatial relationship between lines of O IV and Si IV shows a strong correlation. The correlation coefficient of the turbulent velocity is 0.856 for bright quiet Sun regions. Title: Evolving Active Region Loops Observed with the Transition Region and Coronal explorer. II. Time-dependent Hydrodynamic Simulations Authors: Warren, Harry P.; Winebarger, Amy R.; Mariska, John T. Bibcode: 2003ApJ...593.1174W Altcode: Observations with the Transition Region and Coronal Explorer (TRACE) have revealed a new class of active region loops. These loops have relatively flat filter ratios, suggesting approximately constant temperatures near 1 MK along much of the loop length. The observed apex intensities are also higher than static, uniformly heated loop models predict. These loops appear to persist for much longer than a characteristic cooling time. Recent analysis has indicated that these loops first appear in the hotter Fe XV 284 Å or Fe XII 195 Å filters before they appear in the Fe IX/Fe X 171 Å filter. The delay between the appearance of the loops in the different filters suggests that the loops are impulsively heated and are cooling when they are imaged with TRACE. In this paper we present time-dependent hydrodynamic modeling of an evolving active region loop observed with TRACE. We find that by modeling the loop as a set of small-scale, impulsively heated filaments we can generally reproduce the spatial and temporal properties of the observed loop. These results suggest that both dynamics and filamentation are crucial to understanding the observed properties of active region loops observed with TRACE. Title: Evolving Active Region Loops Observed With TRACE Authors: Warren, H. P.; Winebarger, A. R.; Mariska, J. T. Bibcode: 2003SPD....34.1007W Altcode: 2003BAAS...35Q.826W Recent observations with TRACE have revealed a new class of active region loops with very interesting properties. These loops have relatively flat filter ratios, suggesting approximately constant temperatures along much of the loop length, and large densities relative to the predictions of static loop models. Recent analysis has indicated that these loops first appear in the hotter filters before they appear in the cooler filters. The delay between the appearance of the loops in the different filters suggests that the loops are impulsively heated and are cooling when they are imaged with TRACE. In this paper we present time-dependent hydrodynamic modeling of evolving active region loops observed with TRACE. We find that by modeling the loops as small-scale, impulsively heated filaments we can generally reproduce the spatial and temporal properties of the observations. These results suggest that both dynamics and filamentation are crucial to understanding the observed properties of active region loops observed with TRACE.

This research has been funded by the NASA SR&T and Sun-Earth Connection Guest Investigator programs. Title: Expected Performance of the Extreme Ultraviolet Imaging Spectrometer on Solar-B Authors: Mariska, J. T.; Brown, C. M.; Dere, K. P.; Doschek, G. A.; Korendyke, C. M.; Myers, S. H.; Seely, J. F.; Culhane, J. L.; Watanabe, T. Bibcode: 2003SPD....34.2006M Altcode: 2003BAAS...35..845M The Extreme Ultraviolet Imaging Spectrometer (EIS) is currently under development for flight on the Japanese Solar-B satellite. EIS uses a multilayer-coated off-axis telescope mirror and a multilayer-coated toroidal grating spectrometer to produce stigmatic spectra of solar regions isolated by a 1024 arcsec high slit. The instrument produces monochromatic images either by rastering the solar image across a narrow entrance slit or by using a very wide slit. Half of each optic is coated to optimize reflectance at 19.5 nm, and the other half to optimize reflectance at 27.0 nm, with each wavelength range imaged onto a separate CCD detector.

In this presentation we provide an update on the EIS hardware development and show details of the expected performance of the instrument in solar quiet regions, active regions, and flares. Title: Observing the Dynamic Corona: Diagnostics to Determine Coronal Heating Authors: Winebarger, A. R.; Warren, H. P.; Mariska, J. T. Bibcode: 2003SPD....34.1008W Altcode: 2003BAAS...35R.826W High resolution observations made with TRACE have uncovered a dynamic solar corona. Many of these observations indicate that TRACE is imaging cooling loops (i.e., the loop appears in the TRACE filter sensitive to hotter plasma before it appears in the cooler TRACE filters.) Significant information can be garnered from the TRACE observations. For instance, the delay between the appearance of loop in different filters provides information on the cooling time of the plasma and, hence, the total energy deposited in the loop. The cooling time also indicates a density and hence can be used to determine the degree of filamentation within a loop. TRACE observations of cooling loops, however, tell us little about the spatial and temporal scales for energy deposition. In this talk, we will discuss other diagnostics necessary to pinpoint the magnitude, duration, and location of the heating. The purpose of this talk is to establish the criteria of the necessary spatial, spectral, and temperature resolution necessary to discriminate between the coronal heating theories. Title: Magnetic Modulation of Solar 304 Å Irradiance Authors: Lean, J. L.; Mariska, J. T.; Warren, H. P.; Woods, T. N.; Eparvier, F. G.; McMullin, D. R.; Judge, D. L.; Newmark, J. S.; Viereck, R. A. Bibcode: 2003SPD....34.1902L Altcode: 2003BAAS...35..842L Solar 304 Å irradiance is an important source of heating and ionization in the Earth's upper atmosphere. Because only intermittent observations exist prior to solar cycle 23, the absolute levels and solar cycle variability of 304 Å irradiance are uncertain by a factor of two, based on the range of estimates from four current EUV irradiance variability models. Large active regions are a significant source of 304 Å radiation but their characteristics are not well specified, with contrasts reported in the range of two to ten. Statistical quantification of the role of small scale active regions and network is also lacking. During solar cycle 23, three different instruments are observing the Sun's 304 Å radiation concurrently. The EIT on SOHO records the brightness distribution on the solar disk in a 20 Å band, SEM on SOHO monitors the disk-integrated emission in an 80 Å band, and the SEE grating spectrometer on the TIMED spacecraft recently began observing EUV irradiance spectra with 4 Å resolution. We calculate daily histograms of the brightness distributions of EIT images after adjustments for various instrumental effects. Deconstructions of the histograms permit statistical characterizations of magnetic sources of 304 Å irradiance variability during solar cycle 23, in terms of fractional disk areas and contrasts. We also study center-to-limb variations. The calculations provide independent irradiance variability estimates for comparison with the SEM and SEE direct irradiance observations, and the models. We utilize the source characterizations to revise the NRLEUV model, the present version of which estimates 304 Å emission by assuming that a bright active region has a contrast of ten, and that source region evolution is temporally similar to the Mg chromospheric irradiance index. Funded by NASA SEC GI Program. Title: Transition Region and Coronal Explorer and Soft X-Ray Telescope Active Region Loop Observations: Comparisons with Static Solutions of the Hydrodynamic Equations Authors: Winebarger, Amy R.; Warren, Harry P.; Mariska, John T. Bibcode: 2003ApJ...587..439W Altcode: Active region coronal loop observations with broadband X-ray instruments have often been found to be consistent with the predictions of static loop models. Recent observations in the EUV, however, have discovered a class of active region loops that are difficult to reconcile with static loop models. In this paper, we take a comprehensive look at how coronal loops compare with static models. We select 67 loops with a large range of apex temperatures and half-lengths observed with either the Transition Region and Coronal Explorer or the Soft X-Ray Telescope. We compare these observations to static loop models using both uniform and nonuniform heating. We find that only 2 of the 67 loops are fully consistent with static solutions with uniform heating and a filling factor of unity. We further find that long, cool (<3 MK) loops are as much as 2500 times ``overdense,'' while short, hot (>3 MK) loops are as much as 63 times ``underdense'' when compared to the static solutions with uniform heating. We then consider the possibility that the disparity in the density could be due to steady, nonuniform heating along the loop and find that footpoint heating can increase densities only by a factor of 3 over density solutions with uniform heating while loop-top heating results in density solutions that are, at most, a factor of 2.5 smaller than the density solutions with uniform heating. Only 19 of the 67 loops in this data set could be fully consistent with hydrodynamic solutions with steady heating. Hence, we conclude that static loop models are poor representations of most active region loops. Title: A new model of solar EUV irradiance variability 2. Comparisons with empirical models and observations and implications for space weather Authors: Lean, J. L.; Warren, H. P.; Mariska, J. T.; Bishop, J. Bibcode: 2003JGRA..108.1059L Altcode: Motivated by the need for reliable specification of the Sun's electromagnetic radiation in the extreme ultraviolet (EUV) spectrum, we have developed a new model of solar EUV irradiance variability at wavelengths from 50 to 1200 Å. Solar images are used to quantify changes in the sources of EUV irradiance during the solar cycle. Optically thin EUV emission line fluxes are estimated from differential emission measures (DEMs) that characterize the properties of the solar atmosphere in the source regions, while fluxes for optically thick lines are modeled directly by specifying the source region contrasts. We compare the new model, NRLEUV, with three different empirical models of solar EUV irradiance since 1975. For solar cycles 21 and 22, NRLEUV predicts overall lower EUV irradiances and smaller solar cycle variability than the empirical models. The average total EUV energy at wavelengths from 50 to 1050 Å is 2.9 mW m-2, smaller than the HFG, EUVAC, and SOLAR2000 models for which average energies are 3.7, 4.3, and 5.6 mW m-2, respectively. These differences have distinct wavelength dependencies. The solar cycle variation in total EUV energy is 1.9 for NRLEUV compared with 2.7, 2.9, and 2.3 for HFG, EUVAC, and SOLAR2000. Here, too, the differences are wavelength dependent. We compare both the NRLEUV and the empirically modeled EUV irradiances with selected wavelength bands and emission lines measured during 4 years in cycle 21 by Atmospheric Explorer-E (AE-E) and two broad bands at 170-200 and 260-340 Å measured in cycle 23 by the Solar X-Ray Photometer (SXP) on the Student Nitric Oxide Experiment (SNOE) and the Solar EUV Monitor (SEM) on the Solar and Heliospheric Observatory (SOHO), respectively. The NRLEUV model reproduces the variations observed during solar rotation better than, or as well as, the empirical models. Comparisons of solar cycle variations are more ambiguous because undetected instrumental drifts can cause spurious trends in the observations over these longer timescales. Drifts in the AE-E instruments may explain why the HFG and EUVAC models, which are based on parameterizations of these data, have larger solar cycle variations than NRLEUV. We assess the implications for space weather of the significant differences among the modeled EUV irradiances by using the Atmospheric Ultraviolet Radiance Integrated Code (AURIC) to quantify corresponding differences in upper atmosphere energy deposition and photoionization rates. Title: Overview of the SDO Extreme ultraviolet Variability Experiment (EVE) Authors: Woods, T. N.; Eparvier, F. G.; Rottman, G. J.; Judge, D. L.; McMullin, D. R.; Lean, J. L.; Mariska, J. T.; Warren, H. P.; Berthiaume, G. D.; Bailey, S. M.; Viereck, R. A.; Tobiska, W. K.; Fuller-Rowell, T. J.; Sojka, J. J. Bibcode: 2002AGUFMSH21C..02W Altcode: The NASA Solar Dynamics Observatory (SDO), with its launch in 2007, is the first mission for the NASA Living With a Star (LWS) program. The SDO mission will provide measurements and modeling of the solar radiation and dynamics that can disturb Earth's environment. The Extreme ultraviolet Variability Experiment (EVE) is one of the three instrument suites on SDO. The EVE measures the solar extreme ultraviolet (EUV) irradiance with unprecedented spectral resolution, temporal cadence, accuracy, and precision. Furthermore, the EVE program will incorporate physics-based modeling to advance the understanding of the solar EUV irradiance variations based on the activity of solar magnetic features. The EVE instrument consists of three subsystems. The Multiple EUV Grating Spectrograph (MEGS) measures the 4-120 nm spectral irradiance with 0.1 nm spectral resolution. The Optics Free Spectrometer (OFS), being ionization cells, provides daily, in-flight calibrations for the MEGS channels. The EUV Spectrophotometer (ESP) completes the spectral coverage at 0.1-5 nm and 119-125 nm and provides additional MEGS calibrations. Collectively, the EVE instrument measures the solar EUV irradiance from 0.1 to 125 nm with 7% accuracy and 4% long-term precision. Title: Ionospheric and dayglow responses to the radiative phase of the Bastille Day flare Authors: Meier, R. R.; Warren, H. P.; Nicholas, A. C.; Bishop, J.; Huba, J. D.; Drob, D. P.; Lean, J. L.; Picone, J. M.; Mariska, J. T.; Joyce, G.; Judge, D. L.; Thonnard, S. E.; Dymond, K. F.; Budzien, S. A. Bibcode: 2002GeoRL..29.1461M Altcode: 2002GeoRL..29j..99M The Sun's Bastille Day flare on July 14, 2000 produced a variety of geoeffective events. This solar eruption consisted of an X-class flare followed by a coronal mass ejection that produced a major geomagnetic storm. We have undertaken a study of this event beginning with an analysis of the effects of the radiative phase of the flare on the dayglow and the ionosphere. The key new enabling work is a novel method of evaluating the X-ray and extreme ultraviolet (EUV) solar spectral irradiance changes associated with the flare. We find that the solar radiative output enhancements modeled during the flare are consistent with measurements of both solar EUV irradiance and far UV Earth thermospheric dayglow. We use the SAMI2 model to predict global ionospheric changes along a magnetic meridian that show significantly different northern and southern effects, suggesting that flares can be used to study ionospheric dynamics. Title: The Relationship between SiIV and OIV for Non-thermal Turbulenc Velocity Authors: Akiyama, S.; Doschek, G. A.; Mariska, J. T. Bibcode: 2002AAS...200.3810A Altcode: 2002BAAS...34..700A We report nonthermal turbulence velocities of spectral lines of O IV λ 1401.16 and Si IV λ 1402.77 observed with SUMER spectrometer abord SOHO spacecraft. In ionization equilibrium, the electron temperatures of these ions are 1.6X105 and 6.3X104 K, respectively. Although their spectral line intensities and ratio are vely similar at the quiet area in the lower solar transition region in spite of differential emission measures (Doschek & Mariska 2001). Since these observations help to understand the physical property and the morphology of the transition region, we take note of nonthermal turbulence velocities in this study and compare O IV with Si IV lines using by the observational data of Doschek & Mariska (2001). In order to improve in accuracy, we select the points which error of turbulence velocity are less then 10 % of turbulence velocity both O IV and Si IV line. In the result, the correlation of turbulence velocity between O IV and Si IV is 0.846, we can see strong correlation at the bright points in the quiet region. We discuss the implications of these results for the physical conditions of the transition region. Title: The Structure of the Lower Solar Transition Region Authors: Doschek, G. A.; Mariska, J. T.; Akiyama, S. Bibcode: 2002AAS...200.3811D Altcode: 2002BAAS...34Q.700D Recent high-spatial resolution monochromatic images obtained from the SUMER spectrometer on SOHO have shown that the lower transition region ( 2 x 104 - 2 x 105 K) is composed of small loops and knots of emission (seen on the disk), and thread-like structures (seen above the limb) (Feldman, Widing, & Warren, ApJ, 522, 1133 (1999)). The structures seen in images of different spectral lines formed at significantly different electron temperatures look quite similar. However, because the temperatures are different, the emitting plasma cannot be the same for the different images. What is the physical relationship between lower transition region structures that appear in lines formed at different temperatures? The answer to this question can begin to be addressed by examining SUMER spectra of lower transition region lines formed at different temperatures that appear on the same SUMER exposures. In this case the spatial region on the Sun viewed in both spectral lines is precisely the same, and both lines are recorded simultaneously. The intensity relationship between lines of Si IV (6.3 x 104 K) and O IV (1.3 x 105 K) for such spectra has already been discussed by Doschek & Mariska (ApJ, 560, 420 (2001)), and a strong correlation between Si IV and O IV intensities was found. We will discuss an extension of this work to line groups of, (1) O II, O III (3 x 104, 9.0 x 104 K), (2) C IV, S V, O IV (1 x 105, 1.6 x 105, 1.6 x 105 K), and (3) N IV, O V (1.4 x 105, 2.5 x 105 K). The O II, O III comparison does not show the strong correlation found for higher temperature lines, indicating that chromospheric structures are significantly different from lower transition region structures. The S V and O IV temperature regions strongly overlap but are not identical. Nevertheless, the intensity correlation is quite high. This work was supported by NASA solar physics Guest Investigator Grant S137816. Title: New Determinations of Solar EUV Irradiance Variability for use in the NRLMSIS Atmospheric Density Specification Model Authors: Lean, J. L.; Mariska, J. T.; Warren, H. P.; Bishop, J.; Picone, J. M. Bibcode: 2002AGUSMSH51B..03L Altcode: A variety of space weather models require knowledge of the Sun' s EUV spectral irradiance because this radiation is the predominant source of upper atmosphere heating and ionization. Lacking reliable observations to specify the considerable variability of the EUV spectrum during the solar activity cycle, space weather research and operational models continue to use the 10.7 cm radio flux as a proxy for variations in EUV radiation, even though its shortcomings have been recognized for some time. For example, the largest source of error in special perturbations propagation of spacecraft orbits is the parameterization of solar EUV irradiance in the density models that the codes use to estimate drag. The strongest lines in the EUV spectrum are formed in the Sun' s upper chromosphere whereas the 10.7 cm flux is formed primarily in the hotter corona. We have recently developed a composite chromospheric EUV irradiance index by combining multiple space and ground-based datasets, and are reformulating NRL' s upper atmosphere neutral density model (NRLMSISE-00) to accommodate this new index. In a parallel effort we have developed a new physics-based irradiance variability model (NRLEUV) that calculates the EUV spectrum independently of direct spectral irradiance observations. The model utilizes solar images to extract information about the fraction of the solar atmosphere occupied by different active, network and quiet regions, and coronal holes. Representative differential emission measures are constructed for each of the features and the EUV disk-integrated spectrum is calculated by combining the emission measures with theoretically determined values of plasma emissivity. We use a parameterized version of the NRLEUV model that includes both chromospheric and coronal indices to calculate variations during past solar cycles in the total EUV energy incident at the top of the earth' s atmosphere, and at selected altitude in the range 100 to 1000 km, for use in future reformulations of NRLMSIS. We compare the new chromospheric index and the physics-based EUV irradiance model products with existing EUV model estimates derived from parameterizations of direct observations, and describe how NRLMSIS will incorporate these new determinations of the EUV irradiance to provide an improved density specification for space weather applications. Title: Spectral observations of quiescent EUV loops Authors: Winebarger, A. R.; Mariska, J. T.; Warren, H. P. Bibcode: 2002AAS...200.1603W Altcode: 2002BAAS...34R.667W Recent TRACE observations have detected a class of cool, quiescent loops that are inconsistent with hydrostatic loop models. These loops appear static, isothermal (1 MK), and overdense. In this talk, we present co-aligned TRACE, SUMER and CDS observations of several EUV loops. Every loop observed shows evidence of significant downflows along the loop. We confirm that the temperature along some of the observed loops is sharply peaked around 1 MK. In other loops, however, we find evidence for emission at hotter (2 MK) and cooler (0.2 MK) temperatures; this emission may be co-spatial with the loops observed in TRACE. These observations suggest that non-hydrostatic models are necessary to describe the loops. Title: Energetics of Explosive Events Observed with SUMER Authors: Winebarger, Amy R.; Emslie, A. Gordon; Mariska, John T.; Warren, Harry P. Bibcode: 2002ApJ...565.1298W Altcode: Observations of solar chromosphere-corona transition region plasma show evidence of small-scale, short-lived dynamic phenomena characterized by significant nonthermal broadening and asymmetry in the wings of spectral line profiles. These impulsive mass motions (explosive events) are thought to be the product of magnetic reconnection and to be similar in driving mechanism (though larger in size) to nanoflares, the small-scale events proposed to heat the corona. In this paper, we present a statistical analysis of the energetics of explosive events to address the viability of the nanoflare heating theory. We consider high spectral, spatial, and temporal resolution spectra of the C III λ977, N IV λ765, O VI λ1032, and Ne VIII λ770 lines observed with the Solar Ultraviolet Measurements of Emitted Radiation (SUMER) telescope and spectrometer. Each line profile exhibiting explosive event characteristics was analyzed using the velocity differential emission measure (VDEM) technique. A VDEM is a measure of the emitting power of the plasma as a function of its line-of-sight velocity and hence provides a method of accurately measuring the energy flux associated with an explosive event. We find that these events globally release ~4×104 ergs cm-2 s-1 toward both the corona and chromosphere. This implies that explosive events themselves are not energetically significant to the solar atmosphere. However, the distribution of these explosive events as a function of their energy has a power-law spectral index of α=2.9+/-0.1 for the energy range 1022.7-1025.1 ergs. Since α is greater than 2, the energy content is dominated by the smallest events. Hence, if this distribution is representative of the size distribution down to lower energy ranges (~1022 ergs), such small and (currently) undetectable events would release enough energy to heat the solar atmosphere. Title: The spatial correlation between the non-thermal velocities of different lines in the solar lower transition region Authors: Akiyama, S.; Doschek, G.; Mariska, J. Bibcode: 2002cosp...34E2769A Altcode: 2002cosp.meetE2769A The physical relationship between different temperature regions of the solar transition region is unclear. In an attempt to understand this relationship, we analyze SUMER/SOHO spectra of lines formed at different temperatures that are observed simultaneously at the same locations on the solar disk. The present work concerns the relationship in quiet Sun regions among non-thermal turbulent velocities measured in several spectral lines. For each line, the velocity is determined from the full width at half maximum intensity. To improve the accuracy of the line width measurements, we select data with counting statistics such that the uncertainty in the turbulent velocity is less than 10% of the turbulent velocity. The spatial relationship between lines of O IV1401.16 (1.6 ×105 K) and Si IV1402.77 (6.3 × 104 K) for such spectra shows a strong correlation. The correlation coefficient of the turbulent velocity between O IV and Si IV is 0.784 for bright quiet Sun regions. In this poster we will discuss an extension of this work to line groups of (1) O II, O III (3.2 × 104 , 1.0 × 105 K), (2) N IV, S V, O IV (1.3 × 105 , 1.4 × 105 1.6 × 105 K). The N IV, S V, O IV comparisons also show the correlation. We present these and other results, and discuss the implications for the physical nature of the transition region. Title: Publicly Available Numerical Codes for Modeling the X-ray and Microwave Emissions from Solar and Stellar Activity Authors: Holman, G. D.; Mariska, J. T.; McTiernan, J. M.; Ofman, L.; Petrosian, V.; Ramaty, R. Bibcode: 2001AAS...199.9302H Altcode: 2001BAAS...33.1444H We have posted numerical codes on the Web for modeling the bremsstrahlung x-ray emission and the gyrosynchrotron radio emission from solar and stellar activity. In addition to radiation codes, steady-state and time-dependent Fokker-Planck codes are provided for computing the distribution and evolution of accelerated electrons. A 1-D hydrodynamics code computes the response of the stellar atmosphere (chromospheric evaporation). A code for modeling gamma-ray line spectra is also available. On-line documentation is provided for each code. These codes have been developed for modeling results from the High Energy Solar Spectroscopic Imager (HESSI) along with related microwave observations of solar flares. Comprehensive codes for modeling images and spectra of solar flares are under development. The posted codes can be obtained on NASA/Goddard's HESSI Web Site at http://hesperia.gsfc.nasa.gov/hessi/modelware.htm This work is supported in part by the NASA Sun-Earth Connection Program. Title: The Physics of the Solar Lower Transition Region Authors: Doschek, G. A.; Mariska, J. T. Bibcode: 2001ApJ...560..420D Altcode: We discuss quiet-Sun intensities of spectral lines of O IV λ1401.16 and Si IV λ1402.77, their ratio, and their relation to expected properties of the lower solar transition region. The data consist of simultaneous measurements of the two line intensities for 16,988 pixels with spatial dimensions of 1" square obtained by the Solar Ultraviolet Measurement of Emitted Radiation spectrometer on the Solar and Heliospheric Observatory spacecraft. In ionization equilibrium, the electron temperatures of maximum concentration of the two ions are 1.6×105 and 6.3×104 K, respectively. Assuming ionization equilibrium, the line intensity ratio is directly proportional to the emission measure ratio between plasma at these temperatures. Thus, the observations represent 16,988 snapshots of two temperature regions of the differential emission measure at arcsecond spatial scales in the quiet Sun. We derive an average quiet-Sun λ1401.16/λ1402.77 ratio, acquired from observations over 3 hr and a 30''×290'' spatial region, of 0.267+/-0.050. The 1 σ deviation of this ratio is only 20%, but it is about 2.4 times greater than expected purely from counting statistics. We also find that the ratio is about 20% smaller for the most intense features in the spectra. From analysis of another ratio, i.e., O IV λ1399.77/O IV λ1401.16, we argue that this decrease could be due to a higher electron density in the intense features relative to the lower intensity features. We discuss the implications of these observations for understanding the morphology of the transition region. Title: A new model of solar EUV irradiance variability: 1. Model formulation Authors: Warren, H. P.; Mariska, J. T.; Lean, J. Bibcode: 2001JGR...10615745W Altcode: We present a new model of solar irradiance variability at extreme ultraviolet wavelengths (EUV, 50-1200 Å). In this model, quiet Sun, coronal hole, and active region intensities for optically thin emission lines are computed from emission measure distributions determined from spectrally and spatially resolved observations. For optically thick emission lines and continua, empirical values are used. The contribution of various solar features to the spectral irradiance variability is determined from a simple model of limb-brightening and full-disk solar images taken at the Big Bear Solar Observatory and by the Soft X-Ray Telescope on Yohkoh. To extend our irradiance model beyond the time period covered by the available images, we use correlations with proxies for solar activity. Comparisons with the available irradiance data from the Atmospheric Explorer E (AE-E) spacecraft show that our model is capable of reproducing the rotational modulation of the EUV irradiance near solar maximum. The AE-E data, however, show systematically more solar cycle variability than our model estimates. Title: Solar Flare Particle Acceleration and Atmospheric Response Authors: Miller, J. A.; Mariska, J. T. Bibcode: 2001AGUSM..SH31A09M Altcode: We present initial results from a self-consistent simulation of particle acceleration and atmospheric heating during impulsive solar flares. The simulation code consists of two main components, the UAH SDSPAC (Spatially-Dependent Stochastic Particle Acceleration Code) and the NRL DSFTM (Dynamic Solar Flux Tube Model) code, together with an interface that allows these two components to communicate. Particle acceleration occurs via cascading MHD turbulence. MHD turbulence (consisting of an admixture of fast mode and Alfvén waves) is generated at large scales in the corona and subsequently cascades through the inertial range and into the dissipation range, where it stochastically accelerates both ambient electrons and protons via transit-time and cyclotron resonance, respectively. Both species are energized from thermal to relativistic energies on subsecond timescales. Some of the energetic particles then escape from the corona and enter the chromosphere, where they thermalize through Coulomb collisions. The heated chromosphere then expands into the corona, where the increased density and temperature greatly affect the efficiency of the acceleration process. The highly nonlinear interaction between the acceleration process and the atmospheric response is described by a combined quasilinear and hydrodynamic simulation, based upon the two previously-employed codes above. This is, to our knowledge, the first simulation that acurately takes into account both the micro- and macro-physics of particle acceleration. We present preliminary results such as spatially-dependent energetic particle distributions, coronal temperatures, and densities, and also discuss their application to the spatially-resolved hard and soft X-ray spectra to be obtained from HESSI. This work is supported by NASA Solar Physics SR&T grant NAG5-8480. Title: The Extreme Ultraviolet Imaging Spectrometer on Solar-B Authors: Mariska, J. T.; Brown, C. M.; Dere, K. P.; Doschek, G. A.; Korendyke, C. M.; Culhane, J. L.; Watanabe, T. Bibcode: 2001AGUSM..SH41A12M Altcode: Emission lines in the extreme ultraviolet spectral region provide a sensitive probe of the high-temperature plasma in the solar transition region and corona. Simultaneously achieving high spatial, spectral, and temporal resolution in this wavelength region has been challenging. We describe the design and capabilities of the Extreme Ultraviolet Imaging Spectrometer (EIS) planned for flight on the Japanese Solar-B satellite. EIS consists of a multilayer-coated off-axis telescope mirror and a multilayer-coated toroidal grating spectrometer. The telescope mirror forms a solar image on the spectrometer entrance slit assembly and the spectrometer forms stigmatic spectra of the solar region isolated by the 1024 arcsec high slit. The instrument includes thin-film aluminum filters to reject longer wavelength radiation and CCD detectors at the focal plane. Articulation of the primary mirror provides roughly 1600 arcsec of east-west coarse pointing freedom and 360 arcsec of fine east-west motion for rastering. Monochromatic images are formed either by rastering the solar image across a narrow entrance slit or by using a very wide slit. Half of each optic is coated to optimize reflectance at 19.5 nm, and the other half to optimize reflectance at 27.0 nm. Each wavelength range is imaged onto a separate CCD detector. The EIS spectral range contains emission lines formed over a temperature range from roughly 0.1 to 20 MK. Bright lines in the selected wavelength bands will yield precision measurements of line-of-sight velocities and nonthermal plasma motions. This spectral range also includes several pairs of density-sensitive lines. Title: Ionospheric and Thermospheric Response to Solar Activity on July 14, 2000. Authors: Nicholas, A. C.; Meier, R. R.; Thonnard, S. E.; Dymond, K. F.; Budzien, S. A.; Mariska, J. T.; McCoy, R. P. Bibcode: 2001AGUSM..SA51A07N Altcode: With the launch of the LORAAS sensor aboard the STP/P91-1 ARGOS mission and the follow-on UV sensors on DMSP missions covering the next decade, the scientific and operational communities will be able to assess quantitatively the response of the upper atmosphere to solar and geomagnetic forcing. Coincident observations of solar activity by the LASCO/EIT, CELIAS and SEM instruments aboard SOHO and of the resulting disturbances near Earth by WIND and ACE are analyzed. We report our continuing investigation of the relationships among these sets of observations to determine experimentally the timing and intensity of the thermospheric and ionospheric response to solar-induced geomagnetic forcing. We will focus on the sequence of events beginning with the July 14, 2000 solar flare and ensuing coronal mass ejection. Title: Ionospheric and Thermospheric Effects During the Initial Radiative Phase of the Bastille Day Event Authors: Meier, R. R.; Drob, D. P.; Nicholas, A. C.; Bishop, J.; Picone, J. M.; Thonnard, S. E.; Dymond, K. F.; Budzien, S. A.; Lean, J.; Mariska, J. T.; Huba, J. D.; Joyce, G.; Warren, H. P.; Judge, D. L. Bibcode: 2001AGUSM..SA51A08M Altcode: Increases in the solar EUV and X-ray irradiance during a solar flare can produce enhanced ionization and heating in the terrestrial ionosphere. The resulting energetic photoelectrons in turn cause increases in the far ultraviolet (FUV) dayglow (100 - 150 nm). Enhancements of some 50 per cent had previously been detected in OGO-4 nadir-viewing data [C B Opal, Space Research XIII, 797, 1973]. Similar enhancements have now been seen in the FUV limb-viewing dayglow observations from the ARGOS satellite during the Bastille Day flare (July 14, 2000). Because extinction of the FUV dayglow by O2 prevents seeing below 140 km tangent altitude on the limb, increases in the dayglow above that altitude must be caused by the component of the flare spectral irradiance which is deposited there, namely at wavelengths greater than 20 nm. This conclusion is corroborated by the observation of the flare at 30.3 nm made by the SEM instrument on the SOHO satellite. We study this solar-ionospheric connection using a modified version of the NRL solar spectrum as input to the SAMI2 ionospheric model, and also calculate thermospheric heating rates for this event. Title: Spatially-Dependent Stochastic Acceleration in Solar Flares Authors: Miller, J. A.; Newton, E. K.; Mariska, J. Bibcode: 2000SPD....31.0248M Altcode: 2000BAAS...32Q1291M We present a unified spatially-dependent model for simultaneous ion and electron acceleration in impulsive solar flares. In this model, both particle species are stochastically accelerated out of the thermal distribution and then to relativistic energies via resonance with cascading low-amplitude MHD Alfven and fast mode waves. The coupled and nonlinear wave and particle evolution are treated with a quasilinear simulation, which takes into account additional relevant physical processes such as Coulomb collisions, particle transport and escape, wave transport, and the replenishment of the solar flare acceleration region by a cospatial return current. We demonstrate how electron and ion fluxes consistent with those from a large impulsive event are readily obtained in this acceleration scenario, and consider the spatial dependence of the electron and ion energy-differential distributions. We conclude with the implications for the spatial dependence of the hard X-ray emission. Funded by NASA SEC Solar Physics grant NAG5-8480. 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. Bibcode: 2000IAUTA..24...73F Altcode: No abstract at ADS Title: Analyzing the Energetics of Explosive Events Observed by SUMER on SOHO Authors: Winebarger, Amy R.; Emslie, A. Gordon; Mariska, John T.; Warren, Harry P. Bibcode: 1999ApJ...526..471W Altcode: The SUMER spectrometer on SOHO has obtained numerous observations of optically thin chromosphere-corona transition-region line profiles with high spatial, spectral, and temporal resolution. Many of these profiles exhibit asymmetries and broadenings associated with impulsive mass motions (explosive events) in the solar atmosphere. We present here a new method of analyzing non-Gaussian line profiles to calculate the distribution of fluid velocities and hence the associated energy flux. We illustrate this method through a preliminary analysis of explosive event line profiles observed by SUMER. We derive the magnitudes of the energy fluxes directed both toward and away from the observer, and their (``net flux'') differences. We also identify and quantify the various components of each (i.e., kinetic, thermal and nonthermal enthalpy, and the high-energy component associated with the skewed tail of the distribution). The global energy contribution of explosive events to the solar atmosphere is then estimated under two different ``grouping'' assumptions. This preliminary analysis reveals an average net upward energy flux over the entire Sun of 104-105 ergs cm-2 s-1, up to an order of magnitude larger than previous estimates based on characteristic velocities of the fluid. Furthermore, the global estimate for the separate upward- and downward-directed energy fluxes is 105-106 ergs cm-2 s-1, which is comparable to the energy flux required for heating of the quiet corona and indicates that explosive events may indeed have significant implications for the energy balance of the chromosphere and corona. Title: Concept Study Report: Extreme-Ultraviolet Imaging Spectrometer Solar-B Authors: Doschek, George A.; Brown, Charles M.; Davila, Joseph M.; Dere, Kenneth P.; Korendyke, Clarence M.; Mariska, John T.; Seely, John F. Bibcode: 1999STIN...0011153D Altcode: We propose a next generation Extreme-ultraviolet Imaging Spectrometer (EIS) that for the first time combines high spectral, spatial, and temporal resolution in a single solar spectroscopic instrument. The instrument consists of a multilayer-coated off-axis telescope mirror and a multilayer-coated grating spectrometer. The telescope mirror forms solar images on the spectrometer entrance slit assembly. The spectrometer forms stigmatic spectra of the solar region located at the slit. This region is selected by the articulated telescope mirror. Monochromatic images are obtained either by rastering the solar region across a narrow entrance slit, or by using a very wide slit (called a slot) in place of the slit. Monochromatic images of the region centered on the slot are obtained in a single exposure. Half of each optic is coated to maximize reflectance at 195 Angstroms; the other half to maximize reflectance at 270 Angstroms. The two Extreme Ultraviolet (EUV) wavelength bands have been selected to maximize spectral and dynamical and plasma diagnostic capabilities. Spectral lines are observed that are formed over a temperature range from about 0.1 MK to about 20 MK. The main EIS instrument characteristics are: wavelength bands - 180 to 204 Angstroms; 250 to 290 Angstroms; spectral resolution - 0.0223 Angstroms/pixel (34.3km/s at 195 Angstroms and 23.6 km/s at 284 Angstroms); slit dimensions - 4 slits, two currently specified dimensions are 1" x 1024" and 50" x 1024" (the slot); largest spatial field of view in a single exposure - 50" x 1024"; highest time resolution for active region velocity studies - 4.4 s. Title: Potential Field Source Surface Simulations of Soft X-ray Corona Variability During the Solar Cycle Authors: Lean, J. L.; Wang, Y. -M.; Mariska, J. T.; Acton, L. W. Bibcode: 1999AAS...194.9208L Altcode: 1999BAAS...31..987L Magnetic fields that emerge in the solar photosphere and extend upwards into the corona are associated with coronal heating. Some studies have determined empirically that coronal brightness depends directly on photospheric field strength, whereas others relate the brightness to the length of the loops or to the sheering of opposite polarity fields. We use the potential field source surface (PFSS) model of Wang and Sheeley (ApJ, 392, 310, 1992) to investigate the applicability of a range of quantitative associations between photospheric magnetic fields and the global brightness of the non-flaring soft X-ray corona, recorded in full disk X-rays images made by the SXT on Yohkoh. The model extrapolates all photospheric magnetic field lines, in both active regions and smaller scale features, into the corona. For an assigned coronal temperature of 1.5E6 K, the model determines coronal density by assuming hydrostatic equilibrium along each closed field line and using adopted scaling laws to relate the footpoint density to the magnetic field and/or loop length. Integrating the brightness along the line of sight then permits direct simulation of the independently measured SXT full disk coronal images. With the NSO Carrington magnetic field maps as input, the PFSS simulations can account for 85 global X-ray corona during the six years from 1992 to 1997. This agreement is achieved using a constant coronal temperature and a function that depends on both the absolute strength of the photospheric magnetic field footprints, and on the inverse loop length. Despite the overall good agreement of the simulations and observations, significant differences occur during some Carrington rotations. Simulations that utilize inputs from three independent ground-based observatories (NSO, WSO and MWO) can also at times differ significantly from each other. NASA Office of Space Science has funded this work. Title: A Numerical Package for Modeling Solar Flares and Interpreting HESSI Data Authors: Holman, G. D.; Mariska, J. T.; McTiernan, J. M.; Ofman, L.; Petrosian, V.; Ramaty, R. R. Bibcode: 1999AAS...194.8008H Altcode: 1999BAAS...31..966H HESSI, the High Energy Solar Spectroscopic Imager, will observe the x-ray and gamma-ray emission from solar flares with an unprecedented combination of spectral, spatial, and temporal resolution. The quantitative interpretation of the HESSI data will require a level of numerical modeling not generally demanded by previous observations. In view of this, we are developing an integrated package of modular numeric codes and models for the analysis and interpretation of these data. The package will focus on the energetic electrons produced during the impulsive phase of flares. It will compute both the bremsstrahlung x-ray/gamma-ray emission and the gyrosynchrotron radio emission from model flare configurations and initial electron distributions. Steady-state and time-dependent Fokker-Planck codes will compute the transport of suprathermal electrons. A hydrodynamic code will compute the response of the flare plasma in the model configurations. The proposed computational package will allow for comprehensive modeling of energized electrons in different flare scenarios. The predicted emissions can be compared directly with HESSI and radio images and spectra. The package will provide the necessary framework for comparing electron acceleration models with HESSI data. This work is supported in part by the NASA Sun-Earth Connection Program. Title: Hard and Soft X-Ray Observations of Occulted and Nonocculted Solar Limb Flares Authors: Mariska, John T.; McTiernan, James M. Bibcode: 1999ApJ...514..484M Altcode: Using observations from the Yohkoh Bragg Crystal Spectrometer (BCS), the Soft X-Ray Telescope, and the Hard X-Ray Telescope, we have examined the properties of 45 limb flares. Twenty-eight of the flares appear to have most or all of their footpoints occulted by the solar limb, leaving only soft X-ray emission from a looptop source visible. The remaining 17 flares have exposed footpoints. In most observational characteristics, occulted limb flares are indistinguishable from nonocculted limb flares. There does appear to be some evidence that the peak temperature observed in the BCS Ca XIX channel is lower by 2-3 MK in the occulted flares. We also see some tendency for the hard X-ray spectra averaged over the entire event to exhibit a softer spectral index in the occulted limb flares. Most of the flares for which it is possible to measure a peak in the Ca XIX nonthermal broadening velocity as a function of time show that the peak in the nonthermal broadening velocity occurs after the first significant hard X-ray peak. Title: High-Resolution Observations of the Solar Hydrogen Lyman Lines in the Quiet Sun with the SUMER Instrument on SOHO Authors: Warren, H. P.; Mariska, J. T.; Wilhelm, K. Bibcode: 1998ApJS..119..105W Altcode: We present high-resolution observations of the higher H Lyman series lines taken with the Solar Ultraviolet Measurements of Emitted Radiation (SUMER) experiment flown on the Solar and Heliospheric Observatory (SOHO) spacecraft. We have used systematic observations extending from disk center to the solar limb to compute average profiles for representative solar features of the quiet Sun, limb-brightening curves, and full-disk, quiet-Sun profiles for Lyβ through Lyλ(11) and the Lyman continuum. The effects of radiative transfer are apparent in all of the line profiles we studied. The average quiet-Sun profiles for Lyβ through Lyɛ are self-reversed, and the remaining lines are flat-topped. The characteristics of the line profiles vary markedly with intensity. We observe strong enhancements in the red wings of network profiles, while the faint cell-center profiles are nearly symmetric. We also find that the intensities of the H Lyman lines increase at the limb, although the limb brightening is weak compared to optically thin transition region emission lines and largely obscured by the intensity variations observed in the quiet Sun. Title: A new reference spectrum for the EUV irradiance of the quiet Sun 2. Comparisons with observations and previous models Authors: Warren, H. P.; Mariska, J. T.; Lean, J. Bibcode: 1998JGR...10312091W Altcode: In a companion paper we presented a new reference spectrum for the EUV irradiance of the quiet Sun based primarily on intensities calculated from a quiet Sun emission measure distribution and recent compilations of atomic data. The contributions of optically thick emission lines and continua were included empirically. In this paper we present comparisons between this reference spectrum and independently measured irradiance observations, previous quiet Sun reference spectra, and the predictions of empirical EUV irradiance models. These comparisons indicate relatively good agreement among fluxes of emission lines formed in the solar chromosphere and transition region. The fluxes for coronal emission lines in previous quiet Sun reference spectra, however, do not agree with our calculated fluxes or with a recent irradiance observation taken at a low level of solar activity. Coronal emission lines in the Atmospheric Explorer E (AE-E) quiet Sun reference spectrum SC21REFW have fluxes that are typically smaller than our calculated fluxes by factors of 2 or more. We also identify inconsistencies in the earlier reference spectrum of Heroux and Hinteregger [1978] (F74113), where the fluxes of many coronal emission lines with wavelengths below 250 Å are inconsistent with the fluxes of coronal emission lines at longer wavelengths. The fluxes of EUV continua in the various reference spectra and irradiance observations also differ significantly. Title: A new reference spectrum for the EUV irradiance of the quiet Sun 1. Emission measure formulation Authors: Warren, H. P.; Mariska, J. T.; Lean, J. Bibcode: 1998JGR...10312077W Altcode: We present a quiet Sun irradiance spectrum from 50-1200 Å based primarily on intensities computed from a newly constructed quiet Sun emission measure distribution. We derive the emission measure from a spectrum of a portion of the quiet solar disk measured with the Harvard instrument on Skylab and recent compilations of atomic data. For some specific emission lines and continua which are not optically thin and cannot be computed using an emission measure, we either use intensities from the Harvard spectrum directly or infer them from other observations. Application of a simple center-to-limb variation converts the intensities to equivalent full-disk quiet Sun fluxes. Title: Hydrodynamic Modeling of the Response of the Solar Atmosphere to Bombardment by a Beam of Nonthermal Protons Authors: Emslie, A. Gordon; Mariska, John T.; Montgomery, Michele M.; Newton, Elizabeth K. Bibcode: 1998ApJ...498..441E Altcode: Using a one-dimensional time-dependent numerical hydrodynamic model, we examine the response of the solar atmosphere to heating by a beam of energetic protons with a characteristic energy near 1 MeV. At these energies, the coronal portion of the flaring loop must be treated as a ``warm'' target, while the chromospheric portion behaves as a ``cold'' target. This results in a more uniform heating in the coronal portions of the loop than is the case with energetic electrons, leading to smaller pressure gradients and lower plasma upflow velocities. Such lower velocities would appear at first to be more consistent with observed soft X-ray line profiles. However, velocity differential emission measures computed at various times in the calculation show that heating by energetic protons does not satisfactorily reproduce the atmospheric response as inferred from such observations. Title: The Magnetic Reconnection Explorer (MAGREX) Authors: Schühle, U.; Antionchos, S. K.; Barbee, T. W., Jr.; Bixler, J. V.; Brown, C. M.; Carter, P. H., II; Curdt, W.; Davila, J. M.; Doschek, G.; Feldman, U.; Goldstein, W. H.; Kordas, J.; Lemaire, P.; Mariska, J. T.; Marsch, E.; Moses, J. D.; Seely, J. F.; Wilhelm, K.; Woods, T. N. Bibcode: 1998ESASP.417..289S Altcode: 1998cesh.conf..289S No abstract at ADS Title: VDEM Analysis of Transition Region Line Profiles Observed with the SUMER Instrument on SoHO Authors: Winebarger, A. R.; Warren, H. P.; Emslie, A. G.; Mariska, J. T. Bibcode: 1997AAS...191.7302W Altcode: 1997BAAS...29.1320W The SUMER spectrometer has obtained numerous high spatial and spectral resolution observations of optically-thin transition region line profiles in various solar features (quiet Sun, active region, coronal hole, etc.). Frequently, these line profiles show evidence for both steady and impulsive mass motions, which can have profound implications for the mass and energy balance of the transition region and corona. These motions can be quantified using the Velocity Differential Emission Measure (VDEM) technique to derive the distribution of emission with respect to the line-of-sight velocity. This VDEM distribution can then be used to infer mean plasma velocities, momenta, and energy fluxes. We have found that representations of the energy flux by either the ``mean flow approximation'' {1 / 2}n m{bar v}(3) or by the ``enthalpy approximation''(whether in a purely thermal form nkT {bar v} or incorporating nonthermal turbulence {1 / 2}n m /line {v(2}) {bar v}) all underestimate the true energy flux {1 / 2} n m /line{v(3}) by up to an order of magnitude. In cases where lines formed at different temperatures have been observed in the SUMER spectral range simultaneously, we have estimated the divergence of the energy flux and so the energy deposition rate within the region bounded by the formation heights of the two spectral lines; implications for coronal heating are discussed. This work was supported by grants from the SoHO Guest Investigator Program and by the Office of Naval Research. Title: YOHKOH Bragg Crystal Spectrometer Light Curves for S XV (5.0163 - 5.1143 Angstroms) Authors: Mariska, John T.; Bentley, R. D.; Pike, C. D. Bibcode: 1997STIN...9838248M Altcode: This memorandum report summarizes the data produced during the sixth year of operation by the Bragg Crystal Spectrometer (BCS) on the Yohkoh spacecraft. Each page shows the total count rate in the S XV channel of the BCS for a single day. This channel nominally observes the Sun in the wavelength range from 5.0163 - 5.1143 Angstroms. These plots are useful for identifying flare data for further analysis and for determining the data file name and tape number that contains the data. Title: Observations of Doppler Shifts in a Solar Polar Coronal Hole Authors: Warren, H. P.; Mariska, J. T.; Wilhelm, K. Bibcode: 1997ApJ...490L.187W Altcode: Using observations from the Solar Ultraviolet Measurements of Emitted Radiation experiment flown on the Solar and Heliospheric Observatory spacecraft, we have measured Doppler wavelength shifts in the north polar coronal hole in the 1032 and 1038 Å emission lines of O VI and the 1036 and 1037 Å emission lines of C II relative to chromospheric emission lines. These observations were obtained on 1996 November 2 when the north polar coronal hole boundary extended southward to about 750'' (cosθ=0.65). Our measurements indicate the presence of average net redshifts in coronal holes at temperatures of less than 2.9×105 K. Measurements of systematic wavelength shifts in the Ne VIII resonance lines relative to the quiet Sun suggest a transition to average net outflows near 6.3×105 K in the coronal hole. Title: Observations of Thermal Plasma in a Solar Limb Flare Authors: Mariska, John T.; Doschek, G. A. Bibcode: 1997ApJ...485..904M Altcode: All but a small portion of the top of the 1991 October 21 flare was occulted by the solar limb. Thus, both the Bragg crystal spectrometer (BCS) and the soft X-ray telescope (SXT) on Yohkoh observed only a small region of flaring plasma. Using observations from those instruments, we have determined the temporal behavior of the emission measure, temperature, and nonthermal broadening in the loop-top source. We find that for a portion of the decay phase of this flare, the temperatures determined using the Fe XXV, Ca XIX, and S XV BCS channels and SXT filter ratios all agree. Assuming that the plasma is isothermal, we determine the abundances of Fe XXII, Fe XXIII, and Fe XXIV relative to Fe XXV. Comparing the results with recent ionization equilibrium calculations, we find that there are discrepancies between the Fe XXII-to-Fe XXV ratio, the Fe XXIII-to-Fe XXV ratio, and the Fe XXIV-to-Fe XXV ratio and ionization equilibrium calculations, which we attribute to uncertainties in the ionization balance calculations. Title: Doppler Shifts and Nonthermal Broadening in the Quiet Solar Transition Region: O VI Authors: Warren, H. P.; Mariska, J. T.; Wilhelm, K.; Lemaire, P. Bibcode: 1997ApJ...484L..91W Altcode: Using observations from the Solar Ultraviolet Measurements of Emitted Radiation (SUMER) experiment flown on the Solar and Heliospheric Observatory (SOHO) spacecraft, we have measured Doppler wavelength shifts and nonthermal broadening in the 1032 and 1038 Å emission lines of O VI and the 1036 and 1037 Å emission lines of C II. Near Sun center the C II lines exhibit an average redshift of 2 +/- 3 km s-1, consistent with earlier observations in this temperature range. The O VI emission lines exhibit average Doppler velocities of 5 +/- 3 km s-1, suggesting the presence of redshifted material at 2.9 × 105 K. For the O VI lines, the average nonthermal component of the observed line width is 34 +/- 3 km s-1. Title: Electron Densities in the Solar Polar Coronal Holes from Density-Sensitive Line Ratios of Si VIII and S X Authors: Doschek, G. A.; Warren, H. P.; Laming, J. M.; Mariska, J. T.; Wilhelm, K.; Lemaire, P.; Schühle, U.; Moran, T. G. Bibcode: 1997ApJ...482L.109D Altcode: We derive electron densities as a function of height in the north and south polar coronal holes from a forbidden spectral line ratio of Si VIII. Si VIII is produced at about 8 × 105 K in ionization equilibrium. We also derive densities from a similar line ratio of S X (1.3 × 106 K). The spectra were obtained with the Solar Ultraviolet Measurements of Emitted Radiation spectrometer flown on the Solar and Heliospheric Observatory spacecraft. In addition to the primary mechanism of electron impact excitation, the derivation of theoretical level populations for Si VIII and S X includes both proton and resonance capture excitation. We compare the coronal hole results to quiet-Sun coronal measurements obtained outside the east and west limbs. We find for distances of a few arcseconds outside the solar limb that the average line-of-sight electron densities in the coronal holes are about a factor of 2 lower than in quiet-Sun regions. The decrease of density with height is exponential in the polar holes. We also confirm the result known from a variety of earlier observations that the temperature of most of the plasma in coronal holes does not exceed about 106 K. Title: The Solar Flare Dynamics Imager: A Low-Cost Mission for This Solar Maximum Authors: Wulser, J. -P.; Bruner, M. E.; Strong, K. T.; Canfield, R. C.; Culhane, J. L.; Mariska, J. T.; Polidan, R. Bibcode: 1997SPD....28.0232W Altcode: 1997BAAS...29R.898W The Solar Flare Dynamics Imager (SolFDI) is a very low-cost flare mission proposed for this upcoming solar maximum. It is based on a small solar EUV telescope/spectrograph for Spartan Lite, NASA's new ejectable hitchhiker spacecraft. The experiment's main scientific objective is to investigate the spatial, temporal, and velocity structure of the upflowing hot plasma frequently observed in soft X-ray lines during solar flares. Past observations were spatially unresolved, and the nature of these plasma flows, and their relationship with the impulsive phase flare energy release are not well understood. The second objective is to image the spatial and velocity structure of eruptive flares. Such observations can ultimately reveal the true three-dimensional geometry of the eruptive component of the flare. The Solar Flare Dynamics Imager will observe flares in a few selected extreme ultraviolet lines, including a high temperature Fe XXIV line. The instrument uses normal incidence multilayer coated optics to provide simultaneous imaging and spectroscopy in these lines with good spatial, spectral, and temporal resolution. The instrument is designed to fit within the envelope of the Spartan Lite ejectable hitchhiker spacecraft. Spartan Lite is smaller, and costs a fraction of a SMEX spacecraft. But if launched into the upcoming solar maximum, its 6-12 month mission duration would be sufficient to achieve SolFDI's scientific objectives. Title: Observations of Doppler Shifts and Nonthermal Broadening in the North Polar Coronal Hole and Adjacent Quiet Sun Authors: Mariska, J. T.; Warren, H. P.; Wilhelm, K.; Lemaire, P. Bibcode: 1997SPD....28.0118M Altcode: 1997BAAS...29..882M Coronal holes are thought to be the source of high-speed solar wind streams. It is, however, unclear at what height the outflow of material first becomes apparent. Using the Solar Ultraviolet Measurements of Emitted Radiation (SUMER) experiment on the Solar and Heliospheric Observatory (SOHO), we have obtained observations in the north polar coronal hole, its boundary region, and the adjacent quiet Sun at wavelengths that cover emission lines of O VI at 1032 and 1038 Angstroms, Ne VIII at 770 Angstroms, and Mg X at 625 Angstroms. These lines are formed at temperatures of 0.3, 0.8, and 1.25 MK, respectively, and should thus help to determine the temperature at which outflows are first detected. For O VI and Mg X, we will report on Doppler shift measurements made relative to cooler chromospheric lines. Since there are no suitable emission lines from ions formed in the chromosphere for the Ne VIII line, we are only able to measure relative differences between the coronal hole and the adjacent quiet Sun. We will also report on the magnitude of the nonthermal broadening in these lines in the different solar regions. This work was supported by a NASA SOHO Guest Investigator Program grant. Title: Co-Temporal Evolution of Magnetic Sources of Coronal and Chromospheric/Photospheric Irradiance Variability Authors: Lean, J. L.; Mariska, J. T.; Acton, L. W. Bibcode: 1997SPD....28.1401L Altcode: 1997BAAS...29R.917L Magnetic features emergent from the Sun's convection zone modulate the global radiative output throughout the solar atmosphere. Space-based radiometric monitoring by instruments onboard Yohkoh and UARS have tracked the decline in coronal soft X-rays concurrent with chromospheric and photospheric UV global fluxes from high activity in 1991 to the present solar minimum. Although these different global emissions can at times vary in quite different ways they each exhibit components of variability traceable to common magnetic variability sources, primarily sunspots, bright plages and active network. Comparisons of the SXT soft X-ray images of the corona with groundbased Ca K images of the chromosphere/ photosphere permit the establishment of relationships between these common magnetic sources in solar atmosphere regimes with quite different temperatures and densities. While the impact of large active regions seen in both the coronal and chromospheric images provides the dominant modulation of the emissions (although with different spectral signatures traceable to different spatial scales), more diffuse, extended magnetic sources also contribute to solar cycle changes in the overall background global emission of the corona as well as the chromosphere/photosphere. Title: Doppler Shifts and Nonthermal Broadening in the Quiet Solar Transition Region: O VI Authors: Warren, H. P.; Mariska, J. T.; Wilhelm, K.; Lemaire, P. Bibcode: 1997SPD....28.0117W Altcode: 1997BAAS...29..882W Using observations from the Solar Ultraviolet Measurements of Emitted Radiation (SUMER) experiment flown on the Solar and Heliospheric Observatory (SOHO ) spacecraft, we have measured Doppler wavelength shifts and nonthermal broadening in the 1032 and 1038 Angstroms emission lines of Ovi and the 1036 and 1037 Angstroms emission lines of Cii. Near Sun center the Cii lines exhibit an average redshift of 2+/-3km s(-1) , consistent with earlier observations in this temperature range. The Ovi emission lines exhibit average Doppler velocities of 5+/-3km s(-1) suggesting the presence of redshifted material at 2.9*E(5) K. For the Ovi lines, the average nonthermal component of the observed line width is 34+/-3km s(-1) . These observations indicate a tendency for brighter regions to have larger average redshifts and line widths than faint features although the relationship is very weak. Preliminary analysis of observations at the limb suggests that the Doppler velocities for Ovi do not approach zero as would be expected for predominately radial motions. Title: Determination of the Formation Temperature of Si IV in the Solar Transition Region Authors: Doschek, G. A.; Mariska, J. T.; Warren, H. P.; Wilhelm, K.; Lemaire, P.; Kucera, T.; Schühle, U. Bibcode: 1997ApJ...477L.119D Altcode: Using spectra obtained with the Solar Ultraviolet Measurements of Emitted Radiation (SUMER) spectrometer flown on the Solar and Heliospheric Observatory spacecraft, we deduce the temperature of formation of the Si IV ion in the solar transition region from the Si IV ultraviolet spectral line intensity ratio, 3p 2P3/2-3d 2D3/2,5/2/3s 2S1/2-3p 2P1/2, and compare the result to the temperature predicted under the assumption of ionization equilibrium. The wavelengths are as follows: 2D3/2,5/2, 1128.325, 1128.340 Å 2P1/2, 1402.770 Å. Ratios are derived for typical features of the quiet Sun, such as cell center and network, and are systematically higher than those predicted at the 6.3 × 104 K ionization equilibrium temperature of formation of Si IV. For most solar features the ratios imply a temperature of formation of about 8.5 × 104 K. The ratios for the faintest features imply a temperature of formation of up to 1.6 × 105 K. It is not clear, however, that all the discrepancies between the measured and theoretical ratios are due to a temperature effect. Accurate temperature measurements are important since a large discrepancy from ionization equilibrium has significant implications for the physics of the transition region, such as the possible presence of nonthermal electrons. Title: A Once and Future Stargazer Authors: Mariska, John Bibcode: 1997S&T....93a...6M Altcode: No abstract at ADS Title: The Viability of Energetic Protons as an Agent for Atmospheric Heating during the Impulsive Phase of Solar Flares Authors: Emslie, A. Gordon; Henoux, Jean-Claude; Mariska, John T.; Newton, Elizabeth K. Bibcode: 1996ApJ...470L.131E Altcode: Recent observations of gamma -ray line intensities in solar flares results have led to the suggestion that the energy content in accelerated protons may rival that of accelerated electrons. However, simply having a large energy content in accelerated protons is not sufficient to ensure an important role for protons in driving the response of the atmosphere to flare energy input: a viable model must also deposit a large fraction of the particle energy at the top of the chromosphere to account for the large increase in soft X-ray emission measure that characterizes the main phase of a flare. While hard X-ray producing electrons indeed deposit a sufficient amount of energy at the appropriate depths in the atmosphere, only protons with a characteristic energy of order 1 MeV do likewise. It is intriguing that a characteristic energy of just this value has been obtained through independent analysis of gamma -ray line intensities. However, it must be noted that protons of this energy do not have a signature in hard X-rays, leading us to conclude that a substantial fraction of the flare energy budget must still reside in deka-keV electrons. In order to complete the global energetic picture, further corroborating observational diagnostics for MeV protons are desirable. In this Letter, we discuss such suitable observations. Title: Modeling solar extreme ultraviolet irradiance variability using emission measure distributions Authors: Warren, H. P.; Mariska, J. T.; Lean, J.; Marquette, W.; Johannesson, A. Bibcode: 1996GeoRL..23.2207W Altcode: We introduce a new model of solar irradiance variability at extreme ultraviolet (EUV) wavelengths. The model combines a spectral emission line database, solar emission measure distributions, and estimates from ground-based solar images of the fraction of the Sun covered by the various types of activity to synthesize the irradiance. Using Call K-line images, the model can be used to estimate the irradiance from EUV line emission formed in the upper chromosphere and lower transition region. Comparisons of this new model with existing empirical models reveal both similarities and disagreements in the absolute magnitude, the amplitude of the rotational modulation, and the intermediate-term solar cycle variability of the predicted fluxes. Title: A New Model of Solar EUV Irradiance Variability Authors: Warren, H. P.; Mariska, J. T.; Lean, J. Bibcode: 1996AAS...188.3617W Altcode: 1996BAAS...28R.875W Solar soft X-ray (SXR, 1-100 Angstroms) and extreme ultraviolet (EUV, 100--1200 Angstroms) radiation plays a central role in the energetics and dynamics of the Earth's upper atmosphere. Solar radiation at these wavelengths is strongly affected by solar magnetic activity and varies significantly during the solar activity cycle. Empirical models of solar irradiance variability essentially parameterize existing full-disk irradiance observations with proxies for solar activity. However, the limitations of existing EUV observations and absence of any current irradiance measurements at these wavelengths limits the utility of empirical irradiance modeling. Motivated by solar physics experiments on Yohkoh, SOHO, and TRACE we have developed a new, physics-based approach to modeling solar SXR and EUV irradiance variability. In this new model, the intensities of optically thin spectral lines are calculated using theoretically determined values of plasma emissivity coupled with emission measure distributions for features of the solar atmosphere: coronal holes, quiet Sun, and active regions. For emission lines with very complicated formation processes, such as the Lyman lines of hydrogen and helium, spatially and spectrally resolved solar observations are used in place of emission measure calculations. Information about the distribution of emitting regions on the Sun is inferred from full-disk images of the Sun, such as BBSO CaII k-line and Yohkoh SXT images, rather than from proxies for solar activity. Comparison of the model with existing empirical irradiance models based on F_{10.7} and other proxies for solar activity reveals disagreements in the absolute magnitude, the amplitude of the rotational modulation, and the solar cycle variability of the predicted fluxes at many wavelengths. This research was supported by the NASA SEE program. Title: Energetic Protons as a Form of Energy Transport During The Impulsive Phase of Solar Flares? Authors: Emslie, A. G.; Henoux, J. -C.; Mariska, J. T.; Newton, E. K. Bibcode: 1996AAS...188.2601E Altcode: 1996BAAS...28..857E Recent results based on hard X-ray and gamma-ray observations of solar flares have suggested that the energy content in accelerated protons may rival that of accelerated electrons. However, simply having a large energy content in accelerated protons is not sufficient to ensure an important role for protons in driving the response of the atmosphere to flare energy input: a viable model must also deposit a large fraction of the particle energy at the top of the chromosphere, to account for the large increase in soft X-ray emission measure that characterizes the main phase of a flare. While hard X-ray-producing electrons indeed deposit a sufficient amount of energy at the appropriate depths in the atmosphere, we show that only protons with a characteristic energy of order 1 MeV do likewise. Since protons of this energy do not have a signature in hard X-rays, we conclude that a substantial fraction of the flare energy budget must indeed reside in deka-keV electrons. In order to complete the global energetic picture, observational diagnostics for MeV protons are required; suitable observations are discussed. This work was supported by the NASA Office of Space Science and by the NSF International Programs Division. Title: Observations of Thermal Plasma in a Solar Limb Flare Authors: Mariska, J. T.; Doschek, G. A. Bibcode: 1996AAS...188.7004M Altcode: 1996BAAS...28R.938M While the earliest phases of a solar flare are characterized mainly by nonthermal emissions, such as hard X-rays, the remainder of the event manifests itself primarily as thermal emissions at wavelengths ranging from X-rays through optical. This radiation comes from flare plasma covering a wide range of temperatures. Yohkoh Soft X-Ray Telescope (SXT) observations show that in soft X-rays this emission often comes from complex emitting structures, with temperatures that vary from feature to feature. These temperatures, however, are based on filter ratios and are thus difficult to interpret for a multithermal plasma. Yohkoh Bragg Crystal Spectrometer (BCS) observations also provide a temperature diagnostic for the soft X-ray emitting flare plasma. These temperatures often differ from those obtained using filter ratios, again demonstrating that flare plasma is multithermal. We report on observations of a limb flare observed on 1991 October 21 in which the temperatures measured using emission lines of CaXIX and FeXXV agreed, suggesting that this flare contained substantial amounts of isothermal plasma. We use SXT and BCS data from this flare to verify SXT filter ratio temperatures and to determine relative ion fractions of FeXXII, FeXXIII, FeXIV, and FeXXV for comparison with ionization balance calculations. This work was supported by the NASA Office of Space Science and the Naval Research Laboratory. Title: Hard and Soft X-Ray Observations of Solar Limb Flares Authors: Mariska, John T.; Sakao, T.; Bentley, R. D. Bibcode: 1996ApJ...459..815M Altcode: Using observations from the Yohkoh Bragg Crystal Spectrometer, hard X-ray telescope, and soft X-ray telescope, we have examined eight limb flares. Four of the flares have the footpoints occulted by the solar limb. We find that the occulted flares generally have softer hard X-ray spectra and smaller peak values of the nonthermal broadening velocity than nonocculted flares. All other physical parameters show no differences between occulted flares and nonocculted flares. The hard X-ray spectra support a model in which the footpoint emission is due to thick-target sources, while the looptop emission is due to thin-target sources. High spectral resolution hard X-ray observations should thus show a break in the hard X-ray spectrum of the looptop source. We can find no obvious explanation for the differences in nonthermal broadening velocity. Title: Soft X-Ray Flare Dynamics Authors: Doschek, G. A.; Mariska, John T.; Sakao, T. Bibcode: 1996ApJ...459..823D Altcode: We discuss the dynamics of four soft X-ray flares as revealed by the X-ray resonance line profiles of the He-like ions, Fe xxv, Ca xix, and S xv. The flares chosen for analysis belong to a subclass of events that have intense Doppler blueshifted spectral signatures during the rise phase. The spectra were obtained froin the Bragg crystal spectrometer (BC S) experiment flown on the Japanese Yohkoh spacecraft. We deconvolve the line profiles into a flare decay phase component (stationary component) produced by nonmoving plasma with little or no turbulent motions, and a flare rise phase component (dynamic component) produced by bulk plasma motion and turbulence. The dynamic component is further deconvolved into a high-speed component (greater than 400 km s 1) and a lower speed, more turbulent component. We find that the dynamic and stationary components have approximately the same electron temperature. The dynamic and stationary component fluxes are compared with hard X-ray fluxes obtained from the hard X-ray telescope (HXT) on Yohkoh We find that the onset time of the high-speed dynamic component corresponds closely to the onset of hard X-rays. We discuss the X-ray morphology of the flares as revealed by the soft X-ray telescope (SXT) and hard X-ray telescope (HXT) on Yohkoh. From analysis of the X-ray light curves of individual pixels in the SXT images, we believe we have been able to determine at least some of the locations of the dynamic component in the images. Although the observations support many aspects of chromospheric evaporation models, there are significant problems. No obvious rising fronts of plasma are observed for any of the flares. There are apparent footpoint hard X-ray sources that cannot be physically related in an obvious manner with the main sources of soft X-ray emission. The flares are complex, and therefore there are some ambiguities in interpretation of the morphology. Title: Timing of the soft X-ray blue-wing and the hard X-ray burst from observations by YOHKOH Authors: Bentley, R. D.; Doschek, G. A.; Mariska, J. T. Bibcode: 1996AdSpR..17d..55B Altcode: 1996AdSpR..17...55B A knowledge of the relative timing of the hard X-ray burst and emission in soft X-rays is helpful in deciding between a number of theoretical models that describe the mechanism of a solar flare. Here we continue a study of this relationship using observations from the Yohkoh Bragg Crystal Spectrometer and Hard X-ray Telescope, together with supporting observations from the CGRO Batse experiment. The enhanced capabilities of the instruments onboard Yohkoh have made it possible to study the problem in a way that was not previously possible. A study of the timing, intensity and evolution of the soft X-ray blue-wing shows that there is no simple relationship between hard and soft X-ray emissions; strong blue-wings sometimes result from relatively weak hard X-ray bursts; the burst responsible for the blue wing need not be the first or most intense burst associated with the flare; the blue-wing is found to follow very closely after the hard X-ray burst. We also discuss timing issues and why other researchers may have reached different conclusions on this matter. Title: Testing the Impulsiveness of Solar Flare Heating through Analysis of Dynamic Atmospheric Response Authors: Newton, E. K.; Emslie, A. G.; Mariska, J. T. Bibcode: 1996ApJ...459..804N Altcode: One crucial test of a solar flare energy transport model is its ability to reproduce the characteristics of the atmospheric motions inferred from soft X-ray line spectra. Using a recently developed diagnostic, the velocity differential emission measure (VDEM), we can obtain from observations a physical measure of the amount of soft X-ray mitting plasma flowing at each velocity, v, and hence the total momentum of the upflowing plasma, without approximation or parametric fitting. We have correlated solar hard X-ray emission profiles by the Yohkoh Hard X-ray telescope with the mass and momentum histories inferred from soft X-ray line profiles observed by the Yohkoh Bragg crystal spectrometers. For suitably impulsive hard X-ray emission, an analysis of the hydrodynamic equations predicts a proportionality between the hard X-ray intensity and the second time derivative of the soft X-ray mitting plasma's momentum. This relationship is borne out by an analysis of 18 disk-center impulsive flares of varying durations, thereby lending support to the hypothesis that a prompt energy deposition mechanism, such as an energetic electron flux, is indeed responsible for the soft X-ray response observed in the rise phase of sufficiently impulsive solar flares. Title: YOHKOH Bragg Crystal Spectrometer Light Curves for S XV (5.0163 - 5.1143 A) Authors: Mariska, John T.; Bently, R. D.; Pike, C. D. Bibcode: 1996nrl..rept.....M Altcode: This memorandum report summarizes the data produced during the third year of operation by the Bragg Crystal Spectrometer (BCS) on the Yohkoh spacecraft. Each page shows the total count rate in the S XV channel of the BCS for a single day. This channel nominally observes the Sun in the wavelength range from 5.0163 - 5.1143 A. These plots are useful for identifying flare data for further analysis and for determining the data file name and tape name that contains the data. Title: Magnetic Reconnection in the Solar Atmosphere Authors: Bentley, R. D.; Mariska, J. T. Bibcode: 1996ASPC..111.....B Altcode: 1997ASPC..111.....B The following topics were dealt with: bright points, jets, emerging flux, coronal heating, flare observations, flare theory, larger structures and coronal ejections. Title: YOHKOH observations of solar limb flares Authors: Bentley, R. D.; Mariska, J. T.; Sakao, T. Bibcode: 1996ASPC..109..107B Altcode: 1996csss....9..107B No abstract at ADS Title: Radiative Influences Authors: Mariska, John T.; Lean, Judith Bibcode: 1996ASPC...95..555M Altcode: 1996sdit.conf..555M No abstract at ADS Title: Dynamical Response of the Solar Atmosphere to Flare Heating Authors: Newton, E. K.; Emslie, A. G.; Mariska, J. T. Bibcode: 1996mpsa.conf..559N Altcode: 1996IAUCo.153..559N No abstract at ADS Title: Hard and Soft X-ray Observations of Solar Limb Flares Authors: Mariska, J. T.; Sakao, T.; Bentley, R. D. Bibcode: 1996mpsa.conf..523M Altcode: 1996IAUCo.153..523M No abstract at ADS Title: Relationships between Temperature and Emission Measure in Solar Flares Determined from Highly Ionized Iron Spectra and from Broadband X-Ray Detectors Authors: Feldman, U.; Doschek, G. A.; Mariska, J. T.; Brown, C. M. Bibcode: 1995ApJ...450..441F Altcode: We compare the electron temperature and emission measure of flares at the time of maximum soft X-ray intensity derived using two different techniques: (1) from the ratio of a dielectronic Fe XXIV line to the resonance line of Fe XXV, combined with the absolute intensity of the Fe XXV line, and (2) from the ratio of the 0.5-4.0 Å and 1-8 Å broadband X-ray fluxes, combined with the absolute flux in one of the broadband spectral regions. The high-resolution Fe spectra are obtained with the Bragg Crystal Spectrometer experiment flown on the Japanese Yohkoh spacecraft. The broadband fluxes are obtained from Geostationary Operational Environmental Satellites (GOES). A data set of 540 X-ray magnitude C2 or brighter flares, observed by both spacecraft, is used for the analysis. Both techniques assume an isothermal plasma. The broadband temperatures are substantially lower than the Fe xxv temperatures. We find that the maximum temperature of flares brighter than MS exceeds 2 × 107 K and that the maximum temperature of flares fainter than C4 is substantially lower than 2 × 107 K. We find that the Fe XXV emission measure is linearly proportional to the GOES flux in the 0.5-4.0 Å detector. Title: The Velocity Differential Emission Measure: Diagnostic of Bulk Plasma Motion in Solar Flares Authors: Newton, E. K.; Emslie, A. G.; Mariska, J. T. Bibcode: 1995ApJ...447..915N Altcode: Mass motions are a ubiquitous product of solar flare energy release. A better understanding of the flare plasma's distribution how much is moving and how fast permits insight into the mechanisms of energy transport (and release) which lead to those motions. Observationally, mass motions during flares are often manifested in the shape and location of soft X-ray emission lines. Observed line profiles generally exhibit a width greater than the thermal Doppler width and a blue-wing asymmetry which has been cited as evidence for plasma motions along the line of sight. Past efforts to characterize this excess width and asymmetry have primarily involved the parametric fitting of a double-Gaussian form. In this paper we show, however, that simple two-component models are inconsistent with the observed evolution of spectral lines and hence serve as a poor diagnostic of plasma motions. We therefore generalize the synthesis of line profiles to the case of a continuum of Gaussian components, by introducing a quantity which we term the velocity differential emission measure (VDEM). The VDEM measures the distribution of emission from a volume of plasma as a function of its line-of-sight velocity. It can either be computed from theoretical model atmospheres, or recovered from observed line profiles using an inversion technique. We present the VDEMs of two model flare atmospheres and discuss the differences between them. We also deconvolve a VDEM from a representative Ca XIX flare spectrum observed by the Bragg Crystal Spectrometer instrument aboard Yohkoh Title: Temperature Structure of Active Regions Deduced from the Helium-Like Sulphur Lines Authors: Watanabe, Tetsuya; Haka, Hirohisa; Shimizu, Toshifumi; Hiei, Eijiro; Bentley, Robert D.; Lang, James; Phillips, Kenneth J. H.; David Pike, C.; Fludra, Andrzej; Bromage, Barbara J. I.; Mariska, John T. Bibcode: 1995SoPh..157..169W Altcode: Solar active-region temperatures have been determined from the full-Sun spectra of helium-like sulphur (SXV) observed by the Bragg Crystal Spectrometer on board theYohkoh satellite. The average temperature deduced from SXV is demonstrated to vary with the solar activity level: A temperature of 2.5 × 106 K is derived from the spectra taken during low solar activity, similar to the general corona, while 4 × 106 K is obtained during a higher activity phase. For the latter, the high-temperature tail of the differential emission measure of active regions is found most likely due to the superposition of numerous flare-like events (micro/nano-flares). Title: Hard and Soft X-Ray Observations of Solar Limb Flares Authors: Mariska, J. T.; Sakao, T.; Bentley, R. D. Bibcode: 1995SPD....26.1312M Altcode: 1995BAAS...27..989M No abstract at ADS Title: The Velocity Differential Emission Measure - A Diagnostic of Mass Motions in the Impulsive Phase of Solar Flares Authors: Newton, E. K.; Emslie, A. G.; Mariska, J. T. Bibcode: 1995SPD....26.1206N Altcode: 1995BAAS...27..983N No abstract at ADS Title: Correlated brightness variations in solar radiative output from the photosphere to the corona Authors: Lean, J. L.; Mariska, J. T.; Strong, K. T.; Hudson, H. S.; Acton, L. W.; Rottman, G. J.; Woods, T. N.; Willson, R. C. Bibcode: 1995GeoRL..22..655L Altcode: Correlated brightness variations are shown to occur in time series of coronal soft X-rays exclusive of prominent active regions, chromospheric ultraviolet radiation, and the photospheric total solar irradiance corrected for sunspot effects. These temporal correlations suggest that upwardly extending magnetic fields may have a large scale impact on the solar atmosphere in addition to their demonstrable role of generating localized active regions. The correlations have implications for improving and extending solar spectrum variability models. Title: Cooling of Solar Flare Plasmas. I. Theoretical Considerations Authors: Cargill, Peter J.; Mariska, John T.; Antiochos, Spiro K. Bibcode: 1995ApJ...439.1034C Altcode: Theoretical models of the cooling of flare plasma are reexamined. By assuming that the cooling occurs in two separate phase where conduction and radiation, respectively, dominate, a simple analytic formula for the cooling time of a flare plasma is derived. Unlike earlier order-of-magnitude scalings, this result accounts for the effect of the evolution of the loop plasma parameters on the cooling time. When the conductive cooling leads to an 'evaporation' of chromospheric material, the cooling time scales L5/6/p1/6, where the coronal phase (defined as the time maximum temperature). When the conductive cooling is static, the cooling time scales as L3/4n1/4. In deriving these results, use was made of an important scaling law (T proportional to n2) during the radiative cooling phase that was forst noted in one-dimensional hydrodynamic numerical simulations (Serio et al. 1991; Jakimiec et al. 1992). Our own simulations show that this result is restricted to approximately the radiative loss function of Rosner, Tucker, & Vaiana (1978). for different radiative loss functions, other scaling result, with T and n scaling almost linearly when the radiative loss falls off as T-2. It is shown that these scaling laws are part of a class of analytic solutions developed by Antiocos (1980). Title: Testing the DC-Electric Field Model in a Solar Flare Observed by YOHKOH and the Compton Gamma-Ray Observatory Authors: Zarro, D. M.; Mariska, J. T.; Dennis, B. R. Bibcode: 1995ApJ...440..888Z Altcode: We apply a DC-electric field model to the analysis of soft and hard X-ray observations of a solar flare observed by Yohkoh and the Compton Gamma-Ray Observatory CGRO on 1992 September 6. The flare was observed simultaneously in the soft X-ray Ca XIX line by the Yokhoh Bragg Crystal Spectrometer (BCS) and in hard X-rays (>50 keV) by the CGRO Burst and Transient Spectrometer Experiment (BATSE). A strong stationary component of Ca XIX emission was present at the start of impulsive hard X-ray emission indicating an extended phase of heating prior to the production of energetic nonthermal electrons. We interpret the preflare Ca XIX emission as a signature of Joule heating by field-aligned currents. We relate the temporal variation of impulsive hard X-ray emission to the rate of runaway electron acceleration by the DC-electric field associated with the current. We find that the initial rise in hard X-ray emission is consistent with electron acceleration by a DC-electric field that increased from a preflare value of ≲ 10-5 V cm-1 to (9±1) × 10-5 V cm-1 at the time of the first hard X-ray peak and then remained constant during the rest of the impulsive phase. We attribute the increase in electric field strength to the formation of a current sheet at the reconnection point of two loop structures. The decrease in hard X-ray emission after flare maximum is consistent with a reduction in the number of runaway electrons due to an increase in coronal density produced by chromospheric evaporation. The increased density quenches the runaway process by enhancing collisional thermalization of electrons. To avoid the generation of an unrealistically large magnetic field, the flaring region must be highly filamented into ≳106 oppositely directed current channels of ∼30 cm width with an initial preflare current of ≃3 × 1010 A per channel. Title: YOHKOH Bragg Crystal Spectrometer light curves for CA 29(3.1633 - 3.1933 A): 1 October 1993 - 30 September 1994 Authors: Mariska, John T.; Bentley, R. D.; Pike, C. D. Bibcode: 1994YBCSCrept.....M Altcode: This memorandum report summarizes the data produced during the third year of operation by the Bragg Crystal Spectrometer (BCS) on the Yohkoh spacecraft. Each page shows the total count rate in the Ca XIX channel of the BCS for a single day. This channel nominally observes the Sun in the wavelength range from 3.1633 to 3.1933 A. These plots are useful for identifying flare data for further analysis and for determining the data file name and tape name that contains the data. Title: Jets and brightenings generated by energy deposition in the middle and upper solar chromosphere Authors: Sterling, Alphonse C.; Shibata, Kazunari; Mariska, John T. Bibcode: 1994SSRv...70...77S Altcode: Numerical simulations of energy depositions in the middle and upper solar chromosphere result in ejection of chromospheric material into the corona and heating of the chromospheric gas. These simulations may be capable of describing some of the features seen by the soft X-ray telescope on board theYohkoh satellite. Title: Flare Plasma Dynamics Observed with the YOHKOH Bragg Crystal Spectrometer. II. Properties of the Fe xxv, CA xix, and S XV Resonance Lines Authors: Mariska, John T. Bibcode: 1994ApJ...434..756M Altcode: Using data from the Bragg Crystal Spectrometer (BCS) on the Yohkoh spacecraft, we have computed measures of the total intensity, centroid position, and line widths for the resonance lines of Fe XXV, Ca XIX, and S XV during the rise phase and after maximum for 190 solar flares. The difference between centroid positions early and late in each flare yields a measure of the line-of-sight velocity shift of the line centroids. Roughly 25% of the flares show evidence for spatial shifts of the emitting plasma during the flare. For all three resonance lines in those flares that show only Doppler shifts, we find a trend in the average value of the centroid shift with distance from Sun center suggesting radial mass motions with characteristic velocities of 76, 63, and 58 km/s in the resonance lines of Fe XXV, Ca XIX, and S XV, respectively. For each resonance line there is also a correlation between the rise-phase line widths and the centroid shift. For each resonance line we find no correlation between the centroid shift and the peak intensity, rise time, and total flare duration; and no correlation between the line width and the distance from Sun center, peak intensity, rise time, and total flare duration. Comparing data from the different BCS wavelength channels, we find that the centroid shift in each channel is correlated with the centroid shifts in the other channels. Similarly, the line width in each channel is correlated with the line width in the other channels. Title: The 1991 November 9 Flare at 03.2 UT: Observations from YOHKOH Authors: Doschek, G. A.; Mariska, J. T.; Strong, K. T.; Bentley, R. D.; Brown, C. M.; Culhane, J. L.; Lang, J.; Sterling, A. C.; Watanabe, T. Bibcode: 1994ApJ...431..888D Altcode: We discuss X-ray spectra and soft X-ray images of an M1.9 flare that occurred on 1991 November 9 near 03.2 UT. These data were obtained with instrumentation on the Japanese Yohkoh spacecraft. They cover the entire rise phase and peak flare emission, and the beginning of the decay phase. We determine the dynamics, temperature, and emission measure of the flare as inferred from the X-ray line profiles of resonance lines of Fe XXV, Ca XIX, and S XV. We discuss the morphology of the flare as inferred from the soft X-ray images. The November 9 flare is atypical in that a stronger than usual blueshifted emission component (relative to the stationary component) is observed for the resonance lines at flare onset. We discuss several methods for deconvolving the blueshifted component from the stationary component. The X-ray line profiles are consistent with predictions of numerical simulations of chromospheric evaporation. The X-ray images reveal a flare with a complicated loop geometry that is not fully understood. Many of the features in the images are moving upwards at speeds ranging from a few km/s to about 800 km/s. The blueshifted emission begins near the onset of hard X-ray emission, implying that particle acceleration and upflowing plasma have a common energy source. 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. Bibcode: 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: Studying Solar Flares with YOHKOH and the Compton Gamma-Ray Observatory Authors: Zarro, D.; Mariska, J. T.; Dennis, B. R. Bibcode: 1994kofu.symp..221Z Altcode: We apply a DC-electric field model to the analysis of soft and hard X-ray observations of a solar flare observed by Yohkoh and the Compton Gamma-Ray Observatory on 1992 September 6. The flare was observed in Ca XIX by the Yohkoh Bragg Crystal Spectrometer (BCS) and simultaneously in hard X-rays by the CGRO Burst and Transient Spectrometer Experiment (BATSE). A strong stationary component of Ca XIX emission was observed at the start of impulsive hard X-ray emission indicating an extended phase of heating prior to the production of energetic nonthermal electrons. We interpret the preflare Ca XIX emission as a signature of Joule heating by field-aligned currents. We relate the temporal variation of impulsive hard X-ray emission to the rate of runaway electron acceleration in the same DC-electric field. Title: Book-Review - the Solar Transition Region Authors: Mariska, J. T.; Harper, G.; Jordan, C. Bibcode: 1994Obs...114...58M Altcode: No abstract at ADS Title: A Resonance Line Rations Method for Determining Flare Temperatures Using YOHKOH BCS Spectra Authors: Sterling, A. C.; Doschek, G.; Mariska, J. T.; Hiei, E.; Watanabe, T. Bibcode: 1994xspy.conf..127S Altcode: No abstract at ADS Title: The Correlation of Solar Flare Hard X-Ray Bursts with Doppler Blueshifted Soft X-Ray Flare Emission Authors: Bentley, R. D.; Doschek, G. A.; Simnett, G. M.; Rilee, M. L.; Mariska, J. T.; Culhane, J. L.; Kosugi, T.; Watanabe, T. Bibcode: 1994ApJ...421L..55B Altcode: We have investigated the temporal correlation between hard X-ray bursts and the intensity of Doppler blueshifted soft X-ray spectral line emission. We find a strong correlation for many events that have intense blueshifted spectral signatures and some correlation in events with modest blueshifts. The onset of hard X-rays frequently coincides to within a few seconds with the onset of blueshifted emission. The peak intensity of blueshifted emission is frequently close in time to the peak of the hard X-ray emission. Decay rates of the blueshifted and hard X-ray emission are similar, with the decay of the blueshifted emission tending to lag behind the hard X-ray emission in some cases. There are, however, exceptions to these conclusions, and, therefore, the results should not be generalized to all flares. Most of the data for this work were obtained from instruments flown on the Japanese Yohkoh solar spacecraft. Title: Temperature Structure of Active Regions Deduced from the Helium-Like Sulphur Lines Authors: Watanabe, T.; Hara, H.; Shimizu, T.; Hiei, E.; Mariska, J. T.; Bentley, R. D.; Fludra, A.; Lang, J.; Phillips, K. J. H.; Pike, C. D.; Bromage, B. J. I. Bibcode: 1994xspy.conf...55W Altcode: No abstract at ADS Title: Flare Plasma Dynamics Observed with the YOHKOH Bragg Crystal Spectrometer. I. Properties of the CA XIX Resonance Line Authors: Mariska, John T.; Doschek, G. A.; Bentley, R. D. Bibcode: 1993ApJ...419..418M Altcode: Using data from the Bragg crystal spectrometer on the Yohkoh spacecraft we have computed measures of the total intensity, centroid position, and line width for the resonance line of Ca xix during the rise phase and after maximum for 219 solar flares. The difference between the centroid positions early and late in each flare yields a measure of the line-of-sight velocity shift of the line centroid. We find a trend in the average value of the centroid shift with distance from Sun center suggesting radial mass motions with a characteristic velocity of 58 km s-1. There is a correlation between the rise-phase line widths and the centroid shift. We find no correlation between the centroid shift and the peak intensity, rise time, and total flare duration; and no correlation between the line width and the distance from Sun center, the peak intensity, rise time, and total flare duration. These results do not conclusively support or refute the simple electron-beam-driven model or the thermal model for the rise phase of a solar flare. Title: Testing the Electric Field Model in Solar Flares Authors: Zarro, D. M.; Mariska, J. T.; Dennis, B. R. Bibcode: 1993AAS...183.6803Z Altcode: 1993BAAS...25.1396Z We are analyzing solar flares that show evidence for strong stationary Ca XIX emission at the start of impulsive hard X-rays. An example is an M3.3 event that occurred at 0857 UT on 1992 September 6 in active region AR 7270. The flare was observed in Ca XIX by Yohkoh BCS and simultaneously in hard X-rays by CGRO BATSE. A strong stationary component of Ca XIX emission was already present at the start of impulsive hard X-ray emission, indicating a temperature T ~ 10 times 10(6) K and an emission measure EM ~ 7 times 10(47) cm(-3) . Simultaneous Yohkoh SXT Be-filter images imply a simple loop structure for the main soft X-ray source, with a characteristic cross-sectional area of A ~ 10(17) cm(2) and a half-length L ~ 10(9) cm. The detection of strong stationary soft X-ray emission before the peak of hard X-rays cannot be explained easily by the thick-target driven chromospheric evaporation model. To explain these observations, we adopt a DC-electric field model in which preflare thermal Ca XIX emission is produced by current heating dominating early in the flare, and nonthermal HXR emission is produced by electron runaway acceleration dominating during the impulsive phase. We present a novel method for deriving the strength and temporal variation of the electric field. This work was supported by NASA contracts NAS5-31235 and NAS-32064. Title: The Moments of Ca-XIX Flare Spectra as Model Discriminators Authors: Newton, E.; Emslie, A. G.; Mariska, J. Bibcode: 1993AAS...183.0704N Altcode: 1993BAAS...25.1300N We have measured the moments of Ca-XIX solar flare spectral profiles as observed by the Bragg Crystal Spectrometer aboard the YOHKOH spacecraft. The moments are compared to those calculated for spectra generated from numerical electron-heated model simulations, two-component Gaussian fits, and heat flux models. The comparison permits a test of various theories concerning the dynamics of the solar atmosphere during flares.} Title: YOHKOH Bragg Crystal Spectrometer Observations of Flare Plasma Dynamics Authors: Mariska, J. T. Bibcode: 1993AAS...183.0703M Altcode: 1993BAAS...25.1299M Using data from the Bragg Crystal Spectrometer (BCS) on the Yohkoh spacecraft, I have computed measures of the total intensity, centroid position, and line width for the resonance lines of Fe XXV, Ca XIX, and S XV during the rise phase and after maximum for 190 solar flares. The difference between centroid positions early and late in each flare yields a measure of the line-of-sight velocity shift of the line centroids. Roughly 25% of the flares show evidence for spatial shifts of the emitting plasma during the flare. For all three resonance lines in those flares that show only Doppler shifts, I find a trend in the average value of the centroid shift with distance from Sun center suggesting radial mass motions with characteristic velocities of 76, 63, and 58 km s(-1) in the resonance lines of Fe XXV, Ca XIX, and S XV, respectively. For each resonance line, I find no correlation between the centroid shift and the peak intensity, rise time, and total flare duration; and no correlation between the line width and the distance from Sun center, peak intensity, rise time, and total flare duration. Comparing data from different BCS wavelength channels, I find that the centroid shift in each channel is correlated with the centroid shifts in the other channels. Similarly, the line width in each channel is correlated with the line widths in the other channels. Exploratory model atmosphere calculations suggest that many of these properties can be explained by an electron-beam-heated flare model. This work was supported by the Office of Naval Research. Title: Implications of the Soft X-Ray versus Hard X-Ray Temporal Relationship in Solar Flares Authors: Li, Peng; Emslie, A. Gordon; Mariska, John T. Bibcode: 1993ApJ...417..313L Altcode: We have calculated the time profiles of spatially integrated hard X-ray (30-500 keV) and soft X-ray (1-8 Å) emission in both thick-target electron-heated models, and bulk heated thermal models, of the impulsive phase of solar flares. For the thermal model, we find a serious difficulty: the time profiles of the 30-500 keV hard X-ray emission do not peak at the same time as those for the higher energy component (40-500 keV) of this emission, a result that manifestly disagrees with the observations. In the thick-target model, however, the hard X-ray light curves at all energies >30 keV peak at the same time, lending considerable support to this model.

Observations also suggest that the relationship between the hard X-ray and soft X-ray emission is that of "derivativity," that is, the hard X-ray time profile corresponds not so much to the instantaneous soft X-ray flux, but rather its temporal derivative. We have explored the relationship between the hard X-ray (30-500 keV) and soft X-ray (1-8 Å) time profiles in the thick-target model. Typically we find that the temporal derivative of the soft X-ray emission does indeed correspond well to the instantaneous soft X-ray emission, particularly during the rise phase of the event. The cause of this behavior is a combination of heating and density enhancement processes, and we assess the relative roles of each process for a variety of simple hard X-ray time profiles, ranging from short (5 s rise time) to long (60 s rise-time). As expected, temperature enhancements dominate the behavior for the shortest bursts, with density enhancements becoming important for bursts of greater than approximately 15 s duration. It also appears that some other form of gradual heating (e.g., slow reconnection) persists through the decay phase of the event. Title: The 1992 January 5 Flare at 13.3 UT: Observations from YOHKOH Authors: Doschek, G. A.; Strong, K. T.; Bentley, R. D.; Brown, C. M.; Culhane, J. L.; Fludra, A.; Hiei, E.; Lang, J.; Mariska, J. T.; Phillips, K. J. H.; Pike, C. D.; Sterling, A. C.; Watanabe, T.; Acton, L. W.; Bruner, M. E.; Hirayama, T.; Tsuneta, S.; Rolli, E.; Kosugi, T.; Yoshimori, M.; Hudson, H. S.; Metcalf, T. R.; Wuelser, J. -P.; Uchida, Y.; Ogawara, Y. Bibcode: 1993ApJ...416..845D Altcode: We discuss X-ray spectra and soft X-ray images of an M1.9 flare that occurred on 1992 January 5 near 13.3 UT. These data were obtained with instrumentation on the Japanese Yohkoh spacecraft. They cover the entire rise phase of the flare. To supplement these data we have ground-based magnetograms and Hα spectroheliograms. We calculate the electron temperature and emission measure of the flare as a function of time during the early rise phase using X-ray spectral line intensities and line ratios. Using spectral line widths, line profile asymmetries, and wavelength shifts due to the Doppler effect, we calculate the dynamical properties of the flare. The time development of the morphology of the flare, as revealed by the soft X-ray images and the Hα spectroheliograms, and the physical quantities inferred from the X-ray spectra, are compared with chromospheric evaporation models. There is an enhancement of blueshifted emission that is closely correlated with the hard X-ray bursts. Heating of one loop in the flare is consistent with a conduction-evaporation model, but heating is found in several structures that do not appear to be physically associated with each other. No standard evaporation model can adequately explain all of the observations. Title: Yohkoh observations of plasma upflows during solar flares Authors: Culhane, J. L.; Phillips, A. T.; Pike, C. D.; Fludra, A.; Bentley, R. D.; Bromage, B.; Doschek, G. A.; Hiei, E.; Inda, M.; Mariska, J. T.; Phillips, K. J. H.; Sterling, A. C.; Watanabe, T. Bibcode: 1993AdSpR..13i.303C Altcode: 1993AdSpR..13..303C Observations of two flares, an M 2.2 event on 16 December, 1991 and the precursor to an X1 flare on 15 November, 1991 are presented. Spectra obtained with the Bragg Crystal Spectrometer (BCS) are compared with data from the Hard and Soft X-ray Telescopes (HXT, SXT) and the Wide Band Spectrometer (WBS) on the satellite. For both events the creation of upflowing plasma is detected. While the first event seems to conform well to the chromospheric evaporation model for high temperature plasma production, the behaviour for the second event is more complex. Title: Books-Received - the Solar Transition Region Authors: Mariska, J. T. Bibcode: 1993Sci...261..239M Altcode: No abstract at ADS Title: Upflowing Multimillion Degree Plasma During Solar Flares Authors: Doschek, G. A.; Mariska, J. T.; Rilee, M. Bibcode: 1993BAAS...25R1177D Altcode: No abstract at ADS Title: Flare Plasma Dynamics Observed with the Yohkoh Bragg Crystal Spectrometer Authors: Mariska, J. T.; Doschek, G. A.; Bentley, R. D. Bibcode: 1993BAAS...25Q1178M Altcode: No abstract at ADS Title: A Comparison of Solar Flare Hard X-Ray Bursts with Doppler Blue-Shifted Soft X-Ray Emission Authors: Rilee, M. L.; Bentley, R. D.; Culhane, J. L.; Doschek, G. A.; Mariska, J. T.; Simnett, G. M.; Watanabe, T. Bibcode: 1993BAAS...25.1189R Altcode: No abstract at ADS Title: Studying Flare Models with Yohkoh and GRO/BATSE Authors: Zarro, D.; Mariska, J. T.; Dennis, B. R. Bibcode: 1993BAAS...25.1186Z Altcode: No abstract at ADS Title: Implications of the Soft X-Ray versus Hard X-Ray Temporal Relationship in Solar Flares Authors: Emslie, A. G.; Li, P.; Mariska, J. T. Bibcode: 1993BAAS...25.1196E Altcode: No abstract at ADS Title: Solar Chromospheric and Transition Region Response to Energy Deposition in the Middle and Upper Chromosphere Authors: Sterling, Alphonse C.; Shibata, Kazunari; Mariska, John T. Bibcode: 1993ApJ...407..778S Altcode: A series of numerical simulations modeling the chromosphere and transition region response to deposition of thermal energy ranging from about 5 x 10 exp 24 to 5 x 10 exp 28 ergs in the middle or upper chromosphere is reported. The dissipative effects of heat conduction, optically thin radiation losses in the corona, and an approximate expression for the radiation losses of lower temperature plasma are calculated. In response to the energy deposition, chromospheric material is ejected into the corona in the form of pressure gradient generated jets, jets with pressure-gradient, and shock-generated components, or high-speed gas plugs. Category of ejection depends on the spatial and temporal distribution and the magnitude of the input energy source. Title: YOHKOH Bragg Crystal Spectrometer light curves for CA XIX (3.1631-3.1912A): 1 October 1991 - 30 September 1992 Authors: Mariska, John T.; Bentley, R. D.; Pike, C. D. Bibcode: 1993YBCSCrept.....M Altcode: This Memo Report summarizes the data produced during the first year of operation by the Bragg Crystal Spectrometer (BCS) on the Yohkoh spacecraft. Each page shows the total count rate in the Ca XIX channel of the BCS for a single day. This channel nominally observes the Sun in the wavelength range from 3.1631 to 3.1912 A. These plots are useful for identifying flare data for further analysis and for determining the data file name and tape name that contain the data. Title: Solar Doppler-Shift Measurements in the NE VII 465 Angstrom Emission Line Authors: Mariska, John T.; Dowdy, James F., Jr. Bibcode: 1992ApJ...401..754M Altcode: Using a Dopplergram obtained with the Naval Research Laboratory extreme ultraviolet spectrograph on Skylab, we have searched for Doppler shifts in the Ne VII 465 A emission line, which is formed at a temperature of about 500,000 K. In the quiet sun we find no measurable average Doppler shift to a measurement accuracy of +/- 18 km/s. Small regions of the quiet sun do, however, display measurable Doppler shifts. In active regions, we measure Doppler shifts indicating downflow velocities of up to 70 km/s. Title: Diagnostics of Electron-heated Solar Flare Models. III. Effects of Tapered Loop Geometry and Preheating Authors: Emslie, A. G.; Li, Peng; Mariska, John T. Bibcode: 1992ApJ...399..714E Altcode: A series of hydrodynamic numerical simulations of nonthermal electron-heated solar flare atmospheres and their corresponding soft X-ray Ca XIX emission-line profiles, under the conditions of tapered flare loop geometry and/or a preheated atmosphere, is presented. The degree of tapering is parameterized by the magnetic mirror ratio, while the preheated atmosphere is parameterized by the initial upper chromospheric pressure. In a tapered flare loop, it is found that the upward motion of evaporated material is faster compared with the case where the flare loop is uniform. This is due to the diverging nozzle seen by the upflowing material. In the case where the flare atmosphere is preheated and the flare geometry is uniform, the response of the atmosphere to the electron collisional heating is slow. The upward velocity of the hydrodynamic gas is reduced due not only to the large coronal column depth, but also to the increased inertia of the overlying material. It is concluded that the only possible electron-heated scenario in which the predicted Ca XIX line profiles agree with the BCS observations is when the impulsive flare starts in a preheated dense corona. Title: Observations of Several Small Flares with the Bragg Crystal Spectrometer on YOHKOH Authors: Culhane, J. Leonard; Fludra, Andrzej; Bentley, Robert D.; Doschek, George A.; Watanabe, Tetsuya; Hiei, Eijiro; Lang, James; Carter, Martin K.; Mariska, John T.; Phillips, Andrew T.; Phillips, Kenneth J. H.; Pike, C. David; Sterling, Alphonse C. Bibcode: 1992PASJ...44L.101C Altcode: We have analysed data from two flares of GOES class C7.1 and C8.5 observed by the Yohkoh Bragg Crystal Spectrometer. The high sensitivity of the Yohkoh instrument allows us to observe the very early stages of flare development and to study small events with a high signal-to-noise ratio. Spectral fitting programs have been used to derive plasma temperatures, emission measures and velocities from spectra of S XV, Ca XIX and Fe XXV. Large plasma motions indicative of chromospheric evaporation have been found. A more detailed analysis of a flare which occurred on 1991 October 30 is presented. Title: YOHKOH Bragg Crystal Spectrometer Observations of the Dynamics and Temperature Behavior of a Soft X-Ray Flare Authors: Doschek, George A.; Mariska, John T.; Watanabe, Tetsuya; Hiei, Eijiro; Lang, James; Culhane, J. Leonard; Bentley, Robert D.; Brown, Charles M.; Feldman, Uri; Phillips, Andrew T.; Phillips, Kenneth J. H.; Sterling, Alphonse C. Bibcode: 1992PASJ...44L..95D Altcode: We describe X-ray spectra of an M1.5 flare that occurred on 1991 November 9, starting at about 0313 UT. This flare is unusual in that very intense blueshifted components are observed in the resonance lines of Fe XXV, Ca XIX, and S XV. During the onset of the flare, the resonance lines of Ca XIX and Fe XXV are primarily due to this blueshifted component, which from the Doppler effect indicates line-of-sight speeds and turbulent motions that in combination extend up to 800 km s(-1) . Title: Yohkoh BCS Observations of Doppler Shifts Early in Solar Flares Authors: Mariska, J. T.; Doschek, G. A.; Sterling, A. C.; Culhane, J. L.; Hiei, E.; Watanabe, T.; Lang, J. Bibcode: 1992AAS...180.2308M Altcode: 1992BAAS...24..761M No abstract at ADS Title: Time Variation of Solar Flare Temperatures Determined from YOHKOH BCS Spectra Authors: Sterling, A. C.; Doschek, G. A.; Mariska, J. T.; Pike, C. D.; Culhane, J. L.; Hiei, E.; Watanabe, T.; YOHKOH BCS Team Bibcode: 1992AAS...180.3001S Altcode: 1992BAAS...24..775S Bragg Crystal Spectrometer (BCS) X-ray spectra analysis from past satellite missions indicate that it is possible to estimate temperatures in highly ionized flare plasmas to within about 12\ resonance lines in different He-like ions. This procedure is particularly valuable in cases where other temperature measuring methods are insufficient, such as during the rise phase of flares with strong X-ray spectra blue shifts. Here we examine this ratio variation in several flares using data from the Fe XXV, Ca XIX, and S XV channels of the BCS experiment onboard the Yohkoh satellite. We select flares for which we have good rise phase data, and calibrate the ratios using dielectronic-to-resonance line ratios in selected Fe XXV spectra assuming constant elemental abundances in each event. The Yohkoh BCS is about an order of magnitude more sensitive than previous X-ray flare spectrometers, and is therefore able to examine the early stages of flare development in greater detail than previously possible. For this study we select events for which we have good rise phase data, but data well into the decay phase is available for a number of the selected events. This allows us, for the first time, to follow the evolution of flare spectra from relatively cool temperatures (~ 12 MK in Fe XXV) to previously quoted ``typical" flare temperatures (~ 17 MK in Fe XXV). Title: The solar transition region. Authors: Mariska, J. T. Bibcode: 1992CAS....23.....M Altcode: The solar transition region, which spans the temperature range from 20,000 to 1,000,000K, separates the chromosphere from the corona. All the energy that heats the corona and powers the solar wind must pass through this part of the solar atmosphere. All the mass that goes into the solar wind must flow through it. This book summarizes recent ultraviolet and extreme ultraviolet observations of the transition region, the empirical models derived from them, and the physical models that try to explain both the observations and the empirical models. The observational focus is on quiet solar transition region observations made with Skylab and subsequent rocket and satellite experiments. In addition, the book presents a unified discussion of the analysis of ultraviolet and extreme ultraviolet spectroscopic data, including determination of the emission measure, and density and temperature diagnostics. Title: The Solar Transition Region Authors: Mariska, John T. Bibcode: 1992str..book.....M Altcode: 1993str..book.....M; 1992QB528.M33...... The solar transition region that spans the temperature range from about 20,000 to 1,000,000 K separates the solar chromosphere from the corona. All energy that heats the corona and powers the solar wind must pass through this part of the solar atmosphere. This book summarizes recent ultraviolet and extreme ultraviolet observations of the transition region, the empirical models derived from them, and the physical models that try to explain both the observations and the empirical models. The observational focus is on quiet solar transition region observations made with Skylab and subsequent rocket and satellite experiments. The book also presents a unified discussion of the analysis of ultraviolet and extreme ultraviolet spectroscopic data including the determination of the emission measure and density and temperature diagnostics. This will be useful to astrophysicists who are confronting high-resolution ultraviolet and extreme ultraviolet data from astrophysical plasmas for the first time. Title: The Bragg Crystal Spectrometer for SOLAR-A Authors: Culhane, J. L.; Hiei, E.; Doschek, G. A.; Cruise, A. M.; Ogawara, Y.; Uchida, Y.; Bentley, R. D.; Brown, C. M.; Lang, J.; Watanabe, T.; Bowles, J. A.; Deslattes, R. D.; Feldman, U.; Fludra, A.; Guttridge, P.; Henins, A.; Lapington, J.; Magraw, J.; Mariska, J. T.; Payne, J.; Phillips, K. J. H.; Sheather, P.; Slater, K.; Tanaka, K.; Towndrow, E.; Trow, M. W.; Yamaguchi, A. Bibcode: 1991SoPh..136...89C Altcode: The Bragg Crystal Spectrometer (BCS) is one of the instruments which makes up the scientific payload of the SOLAR-A mission. The spectrometer employs four bent germanium crystals, views the whole Sun and observes the resonance line complexes of H-like FeXXVI and He-like FeXXV, CaXIX, and SXV in four narrow wavelength ranges with a resolving power (λ/Δλ) of between 3000 and 6000. The spectrometer has approaching ten times better sensitivity than that of previous instruments thus permitting a time resolution of better than 1 s to be achieved. The principal aim is the measurement of the properties of the 10 to 50 million K plasma created in solar flares with special emphasis on the heating and dynamics of the plasma during the impulsive phase. This paper summarizes the scientific objectives of the BCS and describes the design, characteristics, and performance of the spectrometers. Title: Numerical Simulations of Microflare Evolution in the Solar Transition Region and Corona Authors: Sterling, Alphonse C.; Mariska, John T.; Shibata, Kazunari; Suematsu, Yoshinori Bibcode: 1991ApJ...381..313S Altcode: Several observers report transient ultraviolet brightenings, often referred to as microflares, in the solar atmosphere. In this paper, the results are presented of a series of one-dimensional numerical simulations examining possible relationships between microflares and the generation of dynamical chromospheric and transition region features. Low-energy and medium-energy microflares eject long-lived cool, dense gas plugs into the corona, with the gas plug traversing the loop apex in the medium energy case. In the case of high-energy microflares, the gas plug is rapidly heated to the temperature of the surrounding corona, and the results resemble the dynamics occurring in standard solar flare thick-target electron beam models. Title: Soft X-Ray Emission from Electron-Beam--heated Solar Flares Authors: Mariska, John T.; Zarro, Dominic M. Bibcode: 1991ApJ...381..572M Altcode: Using time-dependent numerical simulations and Solar Maximum Mission observations of a solar flare on 1985 January 23, a study is conducted of the ability of an electron-beam-heating model to reproduce the rise phase of a flare as observed in soft X-ray lines of Ca XIX. The electron beam is parameterized by a peak flux, a low-energy cutoff, and a spectral index, and has a time dependence similar to the observed hard X-ray burst. For a spectral index of 6, only models with a low-energy cutoff of 20 keV reproduce the observed peak emission in the Ca XIX line complex. All models with a low-energy cutoff of 15 keV produce too much emission, while all models with a 25-keV cutoff too little emission. None of the models reproduces the temporal behavior of the soft X-ray emission. The electron-beam-heated component is theorized to only represent a small fraction of the energy released in the impulsive phase of this flare. Title: Nonequilibrium Ionization Effects in Asymmetrically Heated Loops Authors: Spadaro, D.; Antiochos, Spiro K.; Mariska, J. T. Bibcode: 1991ApJ...382..338S Altcode: The effects of nonequilibrium ionization on magnetic loop models with a steady siphon flow that is driven by a nonuniform heating rate are investigated. The model developed by Mariska (1988) to explain the observed redshifts of transition region emission lines is examined, and the number densities of the ions of carbon and oxygen along the loop are computed, with and without the approximation of ionization equilibrium. Considerable deviations from equilibrium were found. In order to determine the consequences of these nonequilibrium effects on the characteristics of the EUV emission from the loop plasma, the profiles and wavelength positions of all the important emission lines due to carbon and oxygen were calculated. The calculations are in broad agreement with Mariska's conclusions, although they show a significant diminution of the Doppler shifts, as well as modifications to the line widths. It is concluded that the inclusion of nonequilibrium effects make it more difficult to reproduce the observed characteristics of the solar transition region by means of the asymmetric-heating models. Title: Solar Doppler Shift Measurements in the Ne VII 465 Å Emission Line Authors: Mariska, J. T.; Dowdy, J. F., Jr. Bibcode: 1991BAAS...23.1060M Altcode: No abstract at ADS Title: Numerical Studies of Atmospheric Dynamics Driven by Energy Deposition in the Chromosphere Authors: Sterling, A. C.; Mariska, J. T.; Shibata, K. Bibcode: 1991BAAS...23.1029S Altcode: No abstract at ADS Title: Numerical Simulations of Electron-Beam-Heated Solar Flares Authors: Mariska, John T. Bibcode: 1991LNP...387..153M Altcode: 1991fpsa.conf..153M Using time-dependent numerical simulations and Solar Maximum Mission (SMM) observations of a solar flare on 1985 January 23, we examine the ability of an electron-beam-heated model to reproduce the rise phase of a flare as observed in soft X-ray lines of CaXIX. For a spectral index of 6, only models with a low-energy cutoff of 20 keV reproduce the observed peak emission in the CaXIX line complex. None of the models reproduces the temporal behavior of the soft X-ray emission. Title: Numerical Simulations of Ultraviolet and X-ray Microflares Authors: Sterling, A. C.; Shibata, K.; Mariska, J. T. Bibcode: 1991LNP...387...71S Altcode: 1991fpsa.conf...71S A series of numerical simulations indicates that thermal energy releases of 1025 - 1027 ergs in the middle chromosphere can produce ejections into the corona in the form of pressure gradient generated jets, jets with pressure gradient and shock generated components, or high speed gas plugs. Heating of the chromosphere to X-ray emitting temperatures occurs in association with gas plugs, perhaps generating X-ray microflares observable by Solar-A. Chromospheric UV-microflares can occur in association with some jets, but do not generally occur with spicules. Title: Numerical Simulation of Microflare Evolution in the Solar Transition Region and Corona (With 4 Figures) Authors: Sterling, A. C.; Mariska, J. T. Bibcode: 1991mcch.conf..630S Altcode: No abstract at ADS Title: Flare Loop Areas Inferred from Ca XIX Observations Authors: Zarro, D. M.; Mariska, J. T. Bibcode: 1990BAAS...22.1197Z Altcode: No abstract at ADS Title: Dynamic modeling of the solar atmosphere Authors: Mariska, J. T.; Dahlburg, R. B.; Karpen, J. T.; Picone, J. M. Bibcode: 1990EOSTr..71..791M Altcode: A brief review is presented of work done over the last eight years investigating the fundamental physics of plasmas and magnetic fields under conditions similar to those that are thought to be present in the outer layers of the solar atmosphere, including the transition region and the corona. The models used to study the coronal structures and the thermal instability in the solar atmosphere are discussed. The results of studies of magnetic energy release in the corona and MHD turbulence in the solar wind are examined. Title: Numerical Simulations of the Rebound Shock Model for Solar Spicules Authors: Sterling, Alphonse C.; Mariska, John T. Bibcode: 1990ApJ...349..647S Altcode: Using time-dependent numerical simulations, the proposed rebound shock mechanism for spicules has been examined. At temperatures above a critical value, T(c), the radiation is characteristic of the conditions in the optically thin corona and near optically thin transition region. When T less than T(c), the atmosphere has a radiative cooling time, tau(rad) characteristic of chromosphere. The spicule is initiated with a quasi-impulsive force in the low chromosphere, which drives a train of upward propagating rebound shocks along the rigid magnetic flux tube. These shocks then move the transition region upward. The material below the displaced transition region has temperatures and densities similar to those of spicules when T(c) = 20,000 K or more and tau(rad) = 500 s or more, but not when T(c) = 10,000 K, and probably not when tau(rad) = 100 s. For all the cases where the cross sectional area diverges rapidly with height, the upward velocity of the transition region is less than that of spicules. Moreover, the maximum height is less than that of average spicules. Taller, higher velocity spicules result when the magnetic field cross sectional area is constant. In all cases, the rebound shock mechanism produces substantial motions and temperature and density variations in chromospheric and transition region material. It is suggested that this may be a partial explanation for the continuous dynamic state of the lower solar atmosphere. Title: Numerical Simulations of Impulsively Heated Solar Flares Authors: Mariska, John T.; Emslie, A. Gordon; Li, Peng Bibcode: 1989ApJ...341.1067M Altcode: The response of a model solar atmosphere to heating by an electron beam has been studied for electron beam flux spectra which are power laws with low-energy 'knees' (rising linearly with time to a peak at 30 s and then falling linearly to 0 at 60 s) ranging from 10 to 20 keV. The results indicate that high peak electron beam fluxes, low-energy knees, and larger spectral indices all move the atmospheric response toward greater enhancements of the parameters in the coronal regions of the atmosphere. Coronal responses can thus be used as a diagnostic of the parameters of the electron beam. Title: Soft X-Ray Diagnostics of Electron-heated Solar Flare Atmospheres Authors: Li, Peng; Emslie, A. Gordon; Mariska, John T. Bibcode: 1989ApJ...341.1075L Altcode: The dependence of the impulsive-phase Ca XIX w line profile on the form of the flare energy input (assumed to be due to the collisional degradation of a beam of high-energy electrons) is considered. The injected flux spectrum has the form of a power law with a low-energy 'knee', and the effects of varying the total energy flux, spectral index, and knee energy on the w line profile during the impulsive phase have been evaluated. Early in the burst, blueshifts of order 400 km/s are noted, and the peak intensity of the blueshifted component together with spatially unresolved hard X-ray burst spectra can be used to determine the beam filling factor. Title: Soft X-Ray Emission from Electron-Beam-Heated Solar Flares Authors: Mariska, J. T.; Zarro, D. M. Bibcode: 1989BAAS...21..850M Altcode: No abstract at ADS Title: Soft X-Ray Profiles as a Diagnostic of Impulsive Flare Energy Deposition Authors: Emslie, A. G.; Li, P.; Mariska, J. T. Bibcode: 1989BAAS...21..850E Altcode: No abstract at ADS Title: Observational Signatures of Loop Flows Driven by Asymmetric Heating Authors: Mariska, John T. Bibcode: 1988ApJ...334..489M Altcode: Using time-dependent numerical simulations, the author has investigated the observational consequences of highly asymmetric heating in small transition-region loops. The simulations show that, to an observer looking down on the loop, the plasma at C IV - emitting temperatures will appear to be redshifted, as is seen on the Sun. Because of the highly asymmetric location, there will be some cutoff temperature above which the redshifted emission will be replaced by only blueshifted emission. These calculations show that the observation of a blueshifted emission line in the upper transition region of the Sun or other late-type stars may not be evidence for the initial acceleration of the solar wind, but rather just part of a closed circulation system. Title: LASCO: A wide-field white light and spectrometric coronagraph for SOHO Authors: Michels, D. J.; Schwenn, R.; Howard, R. A.; Bartoe, J. -D. F.; Antiochos, S. K.; Brueckner, G. E.; Cheng, C. -C.; Dere, K. P.; Doschek, G. A.; Mariska, J. T. Bibcode: 1988sohi.rept...55M Altcode: The scientific objectives of the LASCO (light and spectrometric coronagraph) project in the SOHO (solar and heliospheric observatory) mission are described. These include investigation of mechanisms for heating of the corona and acceleration of the solar wind, causes of coronal transients, and their role in development of large scale coronal patterns and interplanetary disturbances. The distribution and properties of dust particles, including those released from sun-grazing comets are investigated. Interactions of coronal plasma with the dust are studied. The corona is analyzed spectroscopically by a high-resolution scanning, imaging interferometer. The spectral profiles of three emission lines and one Fraunhofer line are measured for each picture point, giving temperatures, velocities, turbulent motions and volume densities. Polarization analysis yields the direction of coronal magnetic fields. Title: Numerical Simulations of the Rebound Shock Model for Spicules Authors: Sterling, A. C.; Mariska, J. T. Bibcode: 1988BAAS...20Q.989S Altcode: No abstract at ADS Title: Ca XIX X-Ray Emission-Line Signatures of Impulsively Heated Solar Flares Authors: Mariska, J. T. Bibcode: 1988BAAS...20..978M Altcode: No abstract at ADS Title: Helical magnetohydrodynamic turbulence and the coronal heating problem Authors: Dahlburg, R. B.; Dahlburg, J. P.; Mariska, J. T. Bibcode: 1988A&A...198..300D Altcode: Numerical simulations are used to investigate the relaxation of an unconfined, helically turbulent, fully three-dimensional magnetofluid, with conditions similar to those which are thought to result in the heating of the solar corona. In these simulations, the system evolves through a succession of force free states. After a relatively quiescent period of Ohmic decay, a phase of accelerated magnetic energy dissipation occurs. Some magnetic energy is transformed into kinetic energy, and the magnitude of entrophy created is a nontrival fraction of the mean square electric current. Concentrated vorticity structures are seen to play almost as important a role as electric current sheets in the heating process. Coincident with this accelerated dissipation process, a reorganization of the magnetic fields occurs, with transfer of magnetic energy to both shorter and longer wavelength modes than are initially present. The ratio of the magnetic field to the electric current density, alpha does not in general tend to assume a constant value in the force free regions during the evolution of the magnetofluid. Title: Heating-related Flows in Cool Solar Loops Authors: Klimchuk, J. A.; Mariska, J. T. Bibcode: 1988ApJ...328..334K Altcode: The authors have investigated the effects of spatial and temporal variations in the heating of cool loop models in an attempt to explain the net redshifts that are observed on the Sun. In none of the situations considered are the induced flows able to satisfactorily reproduce the observations. In the case of asymmetric heating, the end-to-end flows can be as fast as 20 km s-1, but the downflowing leg is neither appreciably faster nor appreciably brighter than the upflowing leg; no net redshift is produced. In the case of symmetric heating, the downflows can also be large, but they are restricted to temperatures that are well below 105K. Neither situation would give rise to the ⪆7 km s-1 disk-averaged redshifts seen in emission lines of species like C IV. Title: Numerical Simulations of Impulsively Heated Solar Flares Authors: Mariska, J. T.; Emslie, A. G.; Li, P. Bibcode: 1988BAAS...20..715M Altcode: No abstract at ADS Title: Soft X-Ray Diagnostics of Impulsively Heated Solar Flare Atmosphere Authors: Li, P.; Emslie, A. G.; Mariska, J. T. Bibcode: 1988BAAS...20..715L Altcode: No abstract at ADS Title: Influence of Heating Rate on the Condensational Instability Authors: Dahlburg, R. B.; Mariska, J. T. Bibcode: 1988SoPh..117...51D Altcode: We determine by analysis and numerical simulation the effect that various heating rates have on the linear and nonlinear evolution of a typical plasma within a solar magnetic flux tube subject to the condensational instability. We first derive a dispersion relation for infinitesimal disturbances to a condensationally unstable fluid subject to heating rates which are functions of temperature and thermal pressure. This relation leads to an algebraic model for predicting solar flux tube stability in the longwavelength limit as a function of temperature. We find that linear stability depends strongly on the heating rate. We then present the results of numerical simulations of the nonlinear evolution of the condensational instability in a solar magnetic flux tube. Different heating rates lead to quite different nonlinear evolution, as evidenced by the behaviour of the global internal energy. Almost all of the heating rates that we consider produce saturation in bifurcated states, but at somewhat different temperatures and mass densities. Title: A model for the structure and formation of prominences. Authors: Poland, A. I.; Mariska, J. T. Bibcode: 1988dssp.conf..133P Altcode: The authors present a geometric model for the magnetic structure of a prominence inspired by recent high resolution images and magnetic field measurements of filaments and prominences. In this model the observed prominence structures are a mapping of locations in the magnetic field structure where material can condense without falling to the chromosphere. Vertical structures near the footpoints are a series of near potential fields. Title: Solar transition region and coronal response to heating rate perturbations. Authors: Mariska, John T. Bibcode: 1987NASCP2483..117M Altcode: 1987tphr.conf..117M The solar transition region is in a dynamic state characterized by impulsively upflowing plasma and continually downflowing plasma. Using numerical simulations, the conjecture that the areas of downflowing plasma are simply the base regions of coronal loops in which the heating rate is gradually decreasing and the areas of upflowing plasma are the base regions of coronal loops in which the heating rate is gradually increasing is examined. The calculations suggest that gradually reducing or increasing the heating in a magnetic flux tube will not result in plasma motions that are similar to those that are observed at high spatial resolution in the UV. Title: Observational Consequences of Highly Asymmetric Heating in Coronal Loops Authors: Mariska, J. T. Bibcode: 1987BAAS...19.1133M Altcode: No abstract at ADS Title: Production of Heat Energy in a Potential Magnetic Field Authors: Dahlburg, R. B.; Mariska, J. T. Bibcode: 1987BAAS...19.1121D Altcode: No abstract at ADS Title: A Numerical Study of the Nonlinear Thermal Stability of Solar Loops Authors: Klimchuk, J. A.; Antiochos, S. K.; Mariska, J. T. Bibcode: 1987ApJ...320..409K Altcode: A time-dependent numerical model is used to investigate the nonlinear thermal stability of static loops of various heights. Simulations show that the instability of a hot state with loop heights of less than about 1000 km is physically significant, with an initially hot atmosphere in low-lying compact loops evolving to an extended atmosphere with temperatures far below 100,000 K. Results also show that high-lying loops are stable to all reasonable perturbations, including those of large initial amplitude and long wavelength. The simulation results suggest that low-lying compact loops should not be common to the sun, and that cool loops with temperatures near 100,000 K must be formed in the cool state initially and cannot evolve from preexisiting loops. Title: A numerical study of the thermal stability of solar loops. Authors: Klimchuk, J. A.; Antiochos, S. K.; Mariska, J. T. Bibcode: 1987NASCP2483..113K Altcode: 1987tphr.conf..113K An important property of all loops is their thermal stability. If low lying hot loops were thermally unstable, for example, a great majority of the low loops on the Sun might be expected to be cool. How small perturbations evolve in low lying, linearly unstable hot loops was determined and how high lying, linearly stable hot loops respond to large amplitude disturbances such as might be expected on the Sun were examined. Only general descriptions and results are given. Title: Solar Transition Region and Coronal Response to Heating Rate Perturbations Authors: Mariska, John T. Bibcode: 1987ApJ...319..465M Altcode: Observations of Doppler shifts in UV emission lines formed in the solar transition region show continual plasma downflows and impulsive plasma upflows. Using numerical simulations, the authors examine the conjecture that areas of downflowing plasma are the base regions of coronal loops in which the heating is gradually decreasing and that areas of upflowing plasma are the base regions of coronal loops in which the heating rate is gradually increasing. Beginning with a coronal loop in equilibrium, the heating rate is reduced on time scales of 100, 1000, and 2000 s to 10 percent and 1 percent of the initial value, and the loop is allowed to evolve to a new equilibrium. The heating rate for the cooled models is then increased back to the initial value on the same time scales. While significant mass motions do develop in the simulations, both the emission measure and the velocity at 100,000 K do not show the characteristics present in UV observations. Title: Heating Related Flows in Cool Loops Authors: Klimchuk, J. A.; Mariska, J. T. Bibcode: 1987BAAS...19..932K Altcode: No abstract at ADS Title: Nonlinear Evolution of Radiation-driven Thermally Unstable Fluids Authors: Dahlburg, R. B.; DeVore, C. R.; Picone, J. M.; Mariska, J. T.; Karpen, J. T. Bibcode: 1987ApJ...315..385D Altcode: The nonlinear evolution of a radiation-driven thermally unstable planar fluid is simulated numerically using a semiimplicit finite-difference algorithm. When the equilibrium state of the fluid is perturbed by random initial excitation of the velocity field, dense, cool, two-dimensional structures are found to form in a rarer, warmer surrounding medium. The nonlinear phase of evolution is characterized by the turbulent contraction of the condensed region, accompanied by a significant increase in the amount of energy radiated. It is found that, if the random velocity perturbation has a sufficiently large amplitude, the fluid will not form condensed structures. Finally, the relationship of these results to observations of the solar chromosphere, transition region, and corona is discussed. Title: Nonlinear aspects of planar condensational instability Authors: Dahlburg, R. B.; DeVore, C. R.; Picone, J. M.; Mariska, J. T.; Karpen, J. T. Bibcode: 1987STIN...8723565D Altcode: The numerical simulation of the nonlinear evolution of a radiation driven thermally unstable planar fluid, using a semi-implicit finite difference algorithm is discussed. When the equilibrium state of the fluid is perturbed by random initial excitation of the velocity field, dense, cool, two dimensional structures are observed forming in a rarer, warmer, surrounding medium. The nonlinear phase of evolution is characterized by the turbulent contraction of the condensed region, accompanied by a significant increase in the amount of energy radiated. If the random velocity perturbation has a sufficiently large amplitude, the fluid will not form condensed structures. Finally, the relationship of these results to observations of the solar chromosphere, transition region and corona is discussed. Title: A Model for the Structure and Formation of Prominences Authors: Poland, A. I.; Mariska, J. T. Bibcode: 1987dssp.work..133P Altcode: 1987ASSL..150..133P No abstract at ADS Title: Flux Tube Dynamics and Solar/Stellar Redshift Measurements (Invited review) Authors: Mariska, John T. Bibcode: 1987LNP...291...21M Altcode: 1987csss....5...21M; 1987LNP87.291...21M On the Sun and other late-type stars, UV observations show persistent red-shifted profiles in emission lines formed near 105 K in the transition region. These downflows could be the result either of the cooling and downfall of material in coronal loops or of the steady end-to-end flow of plasma in smaller loops. Time-dependent numerical simulations suggest that the steady flow explanation is the most likely. Title: Numerical simulations of a siphon mechanism for quiescent prominence formation. Authors: Poland, A. I.; Mariska, J. T.; Klimchuk, J. A. Bibcode: 1986NASCP2442...57P Altcode: 1986copp.nasa...57P Quiescent prominences represent a significant challenge to our understanding of the flow of mass and energy in the outer layers of the solar atmosphere. A small number of quiescent prominences contain as much mass as the entire corona (Athay, 1976). The problem then is how to get that much material into the relatively small volume of a prominence and maintain it at a temperature of 10,000 K in close proximity to material at one million K. The thermal insulation to conduction provided by the magnetic field explains the disparate temperatures. The mass source problem is less well understood. One method for supplying mass to the prominence is to siphon it from the chromosphere. The siphon mechanism begins with a magnetic loop that evolves into a configuration with a gravitational well, such as that described by Kippenhahn and Schluter (1957). This could be formed, for example, by a twist in the magnetic field. A gravitational well could also be formed by a condensation induced sag in the field. This could further enhance the condensation process. Once this well has formed, or as it is forming, the material in the well area of the loop must cool and condense to the point where radiative losses exceed any heat input. Additional material must also flow into the well from the underlying chromosphere to supply the mass required to form the prominence. One example from a series of numerical simulations that were performed to study the formation of quiescent prominences is presented. Title: A numerical study of the thermal stability of low-lying coronal loops. Authors: Klimchuk, J. A.; Antiochos, S. K.; Mariska, J. T. Bibcode: 1986NASCP2442..389K Altcode: 1986copp.nasa..389K The nonlinear evolution of loops that are subjected to a variety of small but finite perturbations was studied. Only the low-lying loops are considered. The analysis was performed numerically using a one-dimensional hydrodynamical model developed at the Naval Research Laboratory. The computer codes solve the time-dependent equations for mass, momentum, and energy transport. The primary interest is the active region filaments, hence a geometry appropriate to those structures was considered. The static solutions were subjected to a moderate sized perturbation and allowed to evolve. The results suggest that both hot and cool loops of the geometry considered are thermally stable against amplitude perturbations of all kinds. Title: Numerical Simulation of Turbulent Coronal Self-Organization Authors: Dahlburg, R. B.; Dahlburg, J. P.; Mariska, J. T. Bibcode: 1986BAAS...18..901D Altcode: No abstract at ADS Title: Solar Transition Region and Coronal Response to Heating Rate Perturbation Authors: Mariska, J. T. Bibcode: 1986BAAS...18..901M Altcode: No abstract at ADS Title: A Siphon Mechanism for Supplying Prominence Mass Authors: Poland, A. I.; Mariska, J. T. Bibcode: 1986SoPh..104..303P Altcode: We examine a siphon-like mechanism for moving mass from the chromosphere to a gravitational well at the top of a magnetic loop to form a prominence. The calculations assume no apriori flow velocity at the loop base. Instead heating in the loop legs drives the flow. The prominence formation process requires two steps. First, the background heating rate must be reduced to on the order of 1 % of the initial heating rate required to maintain the coronal loop. This forms an initial condensation at the top of the loop. Second, the heating must take place only in the loop legs in order to produce a pressure differential which drives mass up into the well at the top of the loop. The heating rate in the loop must be increased once the prominence has begun to form or full prominence densities can not be achieved in a reasonable time. We conclude that this heating driven siphon-like mechanism is feasible for producing and maintaining prominences. Title: Turbulent Condensation Authors: Dahlburg, R. B.; Picone, J. M.; Mariska, J. T. Bibcode: 1986BAAS...18..676D Altcode: No abstract at ADS Title: A Numerical Study of the Stability of Low-Lying Solar Loops Authors: Mariska, J. T.; Klimchuk, J. A.; Antiochos, S. K. Bibcode: 1986BAAS...18Q.708M Altcode: No abstract at ADS Title: The quiet solar transition region. Authors: Mariska, John T. Bibcode: 1986ARA&A..24...23M Altcode: The results of recent studies (in the UV) of the structure and dynamics of the quiet solar transition region and its role in the mass and energy balance of the outer layers of the solar atmosphere are summarized. The region is one in which temperature increases from 25,000 K to about 1 million K and the matter density, fed by the outward flowing wind and the inward streaming plasma, increases by a factor of 40. The morphology of the region is described, along with the theoretical models being applied to the observed nonthermal line broadening, Doppler wavelength shifts, temporal fluctuations, and fine structure. Deficiencies in existing simple models of the region are discussed. Title: Magnetic energy storage and conversion in the solar atmosphere. Authors: Spicer, D. S.; Mariska, J. T.; Boris, J. P. Bibcode: 1986psun....2..181S Altcode: Contents: Fundamental concepts (magnetic energy generation, ideal MHD theory, non-MHD properties, the concept of "anomalous" resistivity, global electrodynamic coupling). Magnetically controlled energy conversion (magnetic modifications of plasma transport, transition region structure and flows, channeling and acceleration of plasma, channeling and dissipation of MHD waves, anomalous dissipation of field-aligned currents). Magnetohydrodynamic energy conversion (magnetic flux tube emergence, geometric rearrangements, reconnection and magnetic tearing, particle acceleration at a neutral sheet, flare trigger mechanisms). Outstanding questions. Title: On V and hard X-rays, observations and model calculations. Authors: Poland, A. I.; Mariska, J. T. Bibcode: 1986NASCP2449..279P Altcode: 1986rfsf.nasa..279P This paper is an amalgamation of two published works that discuss the observation and theoretical calculations of O V (T ≡ 250,000K) and hard X-rays (30 - 100 keV) emitted during flares. The papers are by Poland et al. (1984, see Abstr. 37.073.132) and Mariska and Poland (1985, see Abstr. 39.076.024). The observations of hard X-rays and O V show that the excitation processes for each type of emission are closely coupled. Except for small differences the two types of emission rise and fall together during a flare. Model calculations are able to reproduce this behavior to a large extent, only when conductive processes do not dominate the energy transport processes. Title: Nonlinear Numerical Simulation of Planar Thermal Instability Authors: Dahlburg, R. B.; DeVore, C. R.; Picone, J. M.; Karpen, J. T.; Mariska, J. T. Bibcode: 1985BAAS...17..833D Altcode: No abstract at ADS Title: Two-Dimensional Nonlinear Numerical Simulations of Thermal Instability in the Solar Atmosphere Authors: Picone, J. M.; Dahlburg, R. B.; DeVore, C. R.; Karpen, J. T.; Mariska, J. T. Bibcode: 1985BAAS...17..843P Altcode: No abstract at ADS Title: Numerical Simulation of a Siphon Mechanism for Quiescent Prominences Authors: Mariska, J. T.; Poland, A. I. Bibcode: 1985BAAS...17..842M Altcode: No abstract at ADS Title: Alfvenic pulses in the solar atmosphere Authors: Mariska, J. T.; Hollweg, J. V. Bibcode: 1985ApJ...296..746M Altcode: Some nonlinear aspects of Alfvenic pulses propagating in coronal loops and the underlying chromosphere are numerically investigated. Heat conduction and radiation are included. The Alfvenic pulses are modeled as axisymmetric twists on a vertical cylindrical flux tube. They nonlinearly couple into acoustic-gravity waves propagating along the flux tube. A single Alfvenic pulse is found to leave two acoustic-gravity pulses in its wake. These pulses can result in significant motions of the transition region and underlying chromosphere. These motions do not resemble spicules, but they may correspond to a variety of observations indicating that the solar atmosphere is in a continual dynamic state. It is suggested that a dynamic chromosphere and transition region may be the inevitable consequence of the coronal heating process itself. Title: The Relation Between Hard X-Ray and Transition Region Line Emission in Solar Flares Authors: Mariska, J. T.; Poland, A. I. Bibcode: 1985SoPh...96..317M Altcode: Observational evidence suggests that both the hard X-ray and ultraviolet emission from the impulsive phase of flares result from an electron beam. We present the results of model calculations that are consistent with this theory. The impulsive phase is envisioned as occurring in many small magnetically confined loops, each of which maintains an electron beam for only a few seconds. This model successfully matches several observed aspects of the impulsive phase. The corona is heated to less than 2 × 106 K, maximum enhanced emission occurs in lines formed near 105 K, and there is only slight enhancement between 105 and 2 × 106 K. The slope of the observed relationship between hard X-ray and OV 1371 Å emission is also matched, but the relative emission is not. The calculations indicate that UV emission lines formed below a temperature of about 105 K will arise predominantly from the chromospheric region heated by the electron beam to transition region temperatures. Emission lines formed at higher temperatures will be produced in the transition region. This should be detectable in density-sensitive line ratios. To account successfully for the impulsive UV emission, the peak temperature in the impulsively heated loops must remain below about 2 × 106 K. Thus our model implies that the impulsive heating takes place in different loops from the hotter gradual phase emission. Title: Alfvénic Pulses in the Solar Atmosphere Authors: Mariska, J. T.; Hollweg, J. V. Bibcode: 1985BAAS...17..643M Altcode: No abstract at ADS Title: Effects of mass motions on solar emission measures inferred from transition-region emission lines Authors: Mariska, J. T. Bibcode: 1984ApJ...281..435M Altcode: Extreme ultraviolet emission line intensities predicted by a numerical model which includes nonequilibrium ionization balance are used as input "observational" intensities to calculate volume emission measures following a standard method which assumes ionization equilibrium. These "observational" emission measures are then compared with the actual emission measure distribution in the atmospheric model. For static equilibrium models, the two sets of emission measures are in good agreement. When mass motions are present, the emission measures calculated from the line intensities differ significantly from the actual values. Title: The energy relation between hard X-ray and O V emission in solar flares Authors: Poland, A. I.; Orwig, L. E.; Mariska, J. T.; Auer, L. H.; Nakatsuka, R. Bibcode: 1984ApJ...280..457P Altcode: The relationship between energy emitted in hard X-rays and the ultraviolet during the impulsive phase of solar flares provides an important diagnostic for understanding the energy flow from nonthermal to thermal. Many flares were observed from the Solar Maximum Mission satellite simultaneously in hard X-rays and the O V line at 1371 A formed at 250,000 K, providing information relevant to this problem. Previous work has shown that short time scale peaks in emission of these two types of radiation coincide in time to within 1 s. In this work the energy relation between the two types of emission is investigated and it is found that for any given flare there is a definite relation between hard X-ray and O V emissions throughout the flare, but from one flare to the next this relation varies markedly. These differences are attributed to the initial conditions in the flaring loops and some exploratory model calculations are presented to support this hypothesis. Title: The Relation Between Hard X-Ray and Transition-Region Line Emission in Solar Flares Authors: Mariska, J. T.; Poland, A. I. Bibcode: 1984BAAS...16R.543M Altcode: No abstract at ADS Title: MHD waves and turbulence in the sun and interplanetary medium. Authors: Barnes, A.; Goldstein, M.; Hollweg, J.; Mariska, J.; Matthaeus, W.; Smith, C.; Smith, E.; Stein, R.; Withbroe, G.; Woo, R. Bibcode: 1984NASRP1120....4B Altcode: Contents: Introduction. Global oscillations of the sun. Observations related to waves or turbulence in the solar atmosphere. Local waves in the solar atmosphere: theoretical considerations. Interplanetary hydromagnetic fluctuations. Recent studies of the interplanetary plasma based on turbulence theory. Effects of waves and turbulence of the solar wind. Title: Effects of Mass Motions on Solar Emission Measures Inferred from Transition Region Emission Lines Authors: Mariska, J. T. Bibcode: 1983BAAS...15..918M Altcode: No abstract at ADS Title: Dynamics and spectroscopy of asymmetrically heated coronal loops Authors: Mariska, J. T.; Boris, J. P. Bibcode: 1983ApJ...267..409M Altcode: Numerical models of steady flows along coronal magnetic flux tubes of varying cross sectional areas are investigated. The flows are induced by altering the spatial symmetry of the heating. In two cases the flux tube geometry is symmetric about the top of the loop, but the spatial dependence of the heating rate is changed from a symmetric deposition which supports a stationary equilibrium to a time-independent asymmetric deposition. In a third case the volumetric heating rate is uniform, but one half of the loop is larger in volume than the other. The resulting velocity structure varies significantly with changes in the flux tube geometry. Calculations of the ionization balance and line emission for a number of ionization stages of oxygen suggest that heating induced flows may be responsible for the redshifts seen in spectral lines formed in the network at transition region temperatures. Title: Relation Between Hard X-ray and OV Energy Emitted During Solar Flares Authors: Poland, A. I.; Orwing, L. E.; Mariska, J. T.; Auer, L. H. Bibcode: 1983BAAS...15..713P Altcode: No abstract at ADS Title: Numerical simulations of loops heated to solar flare temperatures. I Authors: Cheng, C. -C.; Oran, E. S.; Doschek, G. A.; Boris, J. P.; Mariska, J. T. Bibcode: 1983ApJ...265.1090C Altcode: The NRL's Dynamic Flux Tube Model is used to numerically simulate the dynamic response of a coronal magnetic loop to an energy input of the order encountered in solar flares. The coronal plasma is heated by the deposition of flare energy at the top of the loop to more than 10 million K, yielding a conduction front that moves toward the chromosphere, where the plasma is heated by the large downward conductive flux and ablates upward to the coronal part of the loop at velocities of a few hundred km/sec. The conduction front simultaneously produces chromospheric ablation and compresses the material ahead of it. With the aid of compressional instabilities, the compressed plasma grows throughout the flare heating phase, presenting a possible source of the flare optical continuum emission which is correlated with soft X-ray radiation. The observational consequences of rapidly heated loop gas dynamic processes are discussed. In the second part of this presentation, the dynamical calculation results previously obtained are used to predict the spectral line intensities, profiles and wavelengths of several X-ray lines and the UV line of Fe XXI at 1354.1 A. Three different viewing orientations of the loop are considered. Title: Numerical Simulations of Loops Heated to Solar Flare Temperatures - Part Two - X-Ray and Ultraviolet Spectroscopy Authors: Doschek, G. A.; Cheng, C. C.; Oran, E. S.; Boris, J. P.; Mariska, J. T. Bibcode: 1983ApJ...265.1103D Altcode: In the first paper in this series, numerical simulation techniques were used to investigate the fluid dynamics of plasma that is confined to a magnetic flux tube and is heated to solar flare temperatures of about 2 × 107 K. The temperature, density, and velocity of the plasma were derived as functions of position and time in the flux tube or loop, after deposition of flare energy at the top of the loop. In this paper the results of the dynamical calculations described in the first paper in this series are used to predict the spectral line intensities, profiles, and wavelengths of several X-ray lines and the UV line of Fe XXI at 1354.1 Å. The distribution of emission from these lines within the loop is computed, as well as the profiles of the lines that would be recorded by a spectrometer that viewed the entire loop. Three different viewing orientations of the loop are considered. The computed spectra are compared with recent observations obtained from orbiting spacecraft. The computed differential emission measure is flatter than observed, and this result is similar to previous analytical and numerical calculations.

The computed X-ray profiles of Fe xxv and Ca xix lines show a stationary component, i.e., no shift in wavelength due to the Doppler effect, and shifted components produced by ablated chromospheric plasma. These profiles qualitatively resemble some of the X-ray observations. A large Doppler shift of about 0.7 Å is predicted for the Fe XXI line. Such a shift is unobserved in spectra obtained from the Naval Research Laboratory spectrograph on Skylab.

Physically different flare models can apparently produce markedly different spectroscopic results. Differences between computed and observed spectra suggest modifications of the model that might produce better agreement between these quantities and hence result in a better understanding of flare morphology and heating mechanisms. Title: The dynamics of accelerating coronal bullets Authors: Karpen, J. T.; Oran, E. S.; Mariska, J. T.; Boris, J. P.; Brueckner, G. E. Bibcode: 1982ApJ...261..375K Altcode: Results are presented of computer simulations of the jets that accelerate through the corona at velocities of 50 to 400 km/s. Particular emphasis is placed on the sensitivity of the induced acceleration to the form in which energy is put into the system. A comparison is made between the observed and predicted physical characteristics of the high-velocity bullets; the potential contribution of the bullets to the mass and energy balance of the solar corona is considered. It is found that the velocity and temperature evolution of the bullets can be modeled successfully by assuming energy input in the form of an external force, pushing continuously on the ejected material. From the physical characteristics of the model bullets and the energy input required to reproduce the observations, it is concluded that the bullets may constitute a significant fraction of the coronal mass flux but only a negligible component of the coronal energy budget. Title: An explanation for the systematic flow of plasma in the solar transition region Authors: Boris, J. P.; Mariska, J. T. Bibcode: 1982ApJ...258L..49B Altcode: Using numerical simulations, it is shown that the systematic flow of plasma along a coronal magnetic flux tube is easily produced by a change in the spatial dependence of the heating rate from a symmetric deposition which supports a stationary equilibrium to a time-independent asymmetric deposition. The velocity of the flow is roughly proportional to the heating symmetry and is directed to the side of the loop away from the bulk of the energy deposition. Title: A Numerical Simulation of Cooling Coronal Flare Plasma Authors: Doschek, G. A.; Boris, J. P.; Cheng, C. C.; Mariska, J. T.; Oran, E. S. Bibcode: 1982ApJ...258..373D Altcode: We have simulated the cooling of coronal flare plasma (Te > 107 K) using a numerical model of a vertical magnetic flux tube containing an idealized flare chromosphere, transition region, and corona. The model solves the set of one-dimensional, two-fluid hydrodynamic equations. The cooling of the flux tube is calculated for a specific case beginning with an initial atmosphere in hydrostatic equilibrium and a maximum temperature of about 18 × 106 K. The behavior of temperature, density, and velocity is calculated as a function of height as the system cools. Early in the cooling, energy is transported by conduction into the transition region and chromosphere where it is radiated away. Later, the transition region-corona interface moves upward into the tube at velocities of about 20 km s-1, while the chromosphere cools and the coronal component cools by both conduction and radiation. Coronal downflow velocities of about 60 km s-1 are evident during this phase. The expected spectral line emission from the system in X-ray lines of Fe XXV, Fe XXIV, Fe XXII, O VIII, and O VII is also calculated and compared to recent observational results. Some observational results can be explained as a consequence of simple cooling of flare flux tubes. The expected spectral line emission from certain transition region lines is also briefly considered. The dependence of our results on flare size is discussed, and our results are compared with similar previous work. Title: Solar transition region response to variations in the heating rate Authors: Mariska, J. T.; Doschek, G. A.; Boris, J. P.; Oran, E. S.; Young, T. R., Jr. Bibcode: 1982ApJ...255..783M Altcode: The response of a numerical model for the upper chromosphere, transition region, and corona to variations in the energy input has been examined. The numerical model solves the set of one-dimensional two-fluid hydrodynamic equations in a simple vertical magnetic flux tube. The atmosphere responds to both the increase and decrease in energy deposition by smoothly readjusting the temperature gradient and the amount of material in the region of peak radiating efficiency to radiate away energy being deposited. At no time during this readjustment is a departure from a thin laminar transition region structure seen. In addition, a time-dependent description of the nonequilibrium ionization of all of the ionization stages of oxygen has been included. This calculation is coupled with the self-consistent calculations of the dynamical variables. It is found that the nonequilibrium ionization balance calculations for both heating and cooling small loops in the quiet sun predict relative ionic abundances which differ substantially from those which would be predicted by an equilibrium calculation Title: The condensational instability in the solar transition region and corona Authors: Oran, E. S.; Mariska, J. T.; Boris, J. P. Bibcode: 1982ApJ...254..349O Altcode: The stability of plasmas at temperatures and densities typical of the solar transition region and corona is investigated using both a linear analysis and nonlinear time-dependent numerical simulations. Growth rates, decay rates, and oscillation frequencies of the perturbations determined from the linear analysis are in excellent agreement with the simulations. The nonlinear regime is characterized by a bifurcation of the plasma into a cool dense condensation surrounded by a hot tenuous corona. The condensation may then be accelerated by forces in the plasma such as those arising from gravity or differential heating. Finally, the results of the detailed simulation show that the transition region is a dynamically stable structure which is the result of the nonlinear evolution of the condensational instability. Title: Detailed Structure and Energetics of Accelerating Coronal Bullets Authors: Karpen, J. T.; Oran, E. S.; Boris, J. P.; Mariska, J. T. Bibcode: 1982BAAS...14..622K Altcode: No abstract at ADS Title: Dynamic phenomena in coronal flux tubes. Authors: Mariska, J. T.; Boris, J. P. Bibcode: 1982SAOSR.392A..53M Altcode: 1982csss....2...53M The study of stellar atmospheres and the determination of specific physical mechanisms, geometries, and magnetic structures by which coronae are maintained is examined. Ultraviolet and soft X-ray components observed in the radiative output of cool stars and the Sun require counterentropic temperature gradients for their explanation. The existence of a hot corona is recognized as a result of mechanical or fluid dynamic effects and the importance of the magnetic field in the heating is accepted. Magnetohydrodynamic energy release associated with the emergence of magnetic flux through the chromosphere and its dynamic readjustment in the corona are major counterentropic phenomena which are considered as primary candidates for corona heating. Systematic plows in coronal flux tubes result from asymmetric heating and systematic flows can exist without substantial chromospheric pressure differences. Title: The E and F region ionospheric response to solar flares: 1. Effect of approximations of solar flare EUV fluxes Authors: Mariska, J. T.; Oran, E. S. Bibcode: 1981JGR....86.5868M Altcode: SOLRAD and many other satellite systems have provided a large data base showing the time-dependent behavior of broadband solar fluxes in the X-ray and EUV spectral regions. These bands are broad in the sense that one band may contain many ionospherically important spectral lines. We present results of tests performed to determine how this information can best be used to predict the effects of a solar flare on the ionosphere. Our approach has been to first adopt a model of the spectral line and continuum enhancements based on a synthesis of many types of flare observations. This detailed spectral model is used in a time-dependent ionosphere model to calculate the response of the electron and ion density profiles. Then the spectral model is mathematically filtered to show how it would appear to the SOLRAD EUV detectors, and this degraded information is used in the ionosphere model. Comparison of the two ionosphere calculations shows that the two spectra produce changes in the total electron content in the ionosphere that differ by only a few percent. Thus, given the present uncertainty in our knowledge of solar flare EUV spectra, SOLRAD broadband EUV solar flux measurements can be used to calculate the ionospheric effects of EUV flare enhancements. Significant changes due to the flare which occur in the individual species densities are described. Title: Mass motions in optically thin solar transition zone lines Authors: Doschek, G. A.; Mariska, John T.; Feldman, U. Bibcode: 1981MNRAS.195..107D Altcode: The widths of optically thin EUV spectral lines formed at temperatures between ≃ 3 × 104 and 2 × 105 K in the solar transition zone are larger than expected assuming ionization equilibrium. This result has been interpreted as due to non-thermal mass motions, characterized by a parameter ξ(km s-1) In this paper we discuss observations of spectral line recorded mostly at +2 arcsec outside the limb of the north and south polar coronal holes, and compare the derived values of ξ to values deduced from spectra of quiet Sun regions. These spectra were recorded by the NRL spectrograph on Skylab (1100-2000 Å). Systematic differences in line widths between coronal holes and quiet Sun region spectra are probably no larger than 0.01 Å, for the optically thin lines used in the analysis. -sight path lengths of the emitting plasma at 2 arc sec above the limb are calculated from the intensity ratios of optically thick lines of C IV, N V, Al III, and Si IV. These ratios should be 2:1 in the optically thin limit, but they are around 1.5 at 2 arcsec above the solar limb. The derived path lengths range from ≃1000 to 5000km. Title: The Dynamics of Coronal Flare Loops: II. Comparison to Observations Authors: Doschek, G. A.; Cheng, C. -C.; Boris, J. P.; Mariska, J. T.; Oran, E. S. Bibcode: 1981BAAS...13..819D Altcode: No abstract at ADS Title: The Dynamics of Accelerating Coronal Bullets Authors: Karpen, J. T.; Oran, E. S.; Boris, J. P.; Mariska, J. T.; Brueckner, G. E. Bibcode: 1981BAAS...13..913K Altcode: No abstract at ADS Title: The Dynamics of Coronal Flare Loops: I. Gasdynamics Authors: Cheng, C. -C.; Doschek, G. A.; Boris, J. P.; Mariska, J. T.; Oran, E. S. Bibcode: 1981BAAS...13Q.819C Altcode: No abstract at ADS Title: Solar Transition Region Response to Heating Rate Variations Authors: Oran, E. S.; Mariska, J. T.; Boris, J. P.; Young, T. R.; Doschek, G. A. Bibcode: 1981BAAS...13..836O Altcode: No abstract at ADS Title: Mass Flows in the Solar Corona as a Diagnostic of the Coronal Heating Function Authors: Mariska, J. T.; Boris, J. P. Bibcode: 1981BAAS...13..836M Altcode: No abstract at ADS Title: The detection of companion stars to the Cepheid variables Eta Aquilae and T Monocerotis. Authors: Mariska, J. T.; Doschek, G. A.; Feldman, U. Bibcode: 1981NASCP2171..209M Altcode: 1981NASCP3171..209M; 1980IUE80......209M; 1981uviu.nasa..209M Ultraviolet spectra of the classical Cepheid variables eta Aq1 and T Mon at several phases in their periods were obtained with IUE. For eta Aq1 significant ultraviolet emission is detected at wavelengths less than 1600 A, where little flux is expected from classical Cepheids. Furthermore, the emission at wavelengths less than about 1600 A does not vary with phase. Comparison with model atmosphere flux distributions shows that the nonvariable emission is consistent with the flux expected from a main sequence companion star with an effective temperature of about 9500 K (AO V - A1 V). For T Mon a nonvarying component to the ultraviolet emission is observed for wavelengths less than 2600 A. Comparison with model atmosphere flux distributions suggests that the companion has an effective temperature of around 10,000 K (AO) and is near the main sequence. Title: The ionospheric response to solar flares. 1: Effects of approximations of solar flare EUV fluxes Authors: Oran, E. S.; Mariska, J. T. Bibcode: 1981STIN...8117976O Altcode: SOLRAD and many other satellite systems have provided a large data base showing the time-dependent behavior of broad and band solar fluxes in the X-ray and EUV spectral regions. These bands are broad in the sense that one band may contain many ionospherically important spectral lines. We present results of tests performed to determine how this information can be best be used to predict the effects of a solar flare on the ionosphere. Our approach has been to first adopt a model of the spectral line and continuum enhancements based on a synthesis of many types of flare observations. This detailed spectral model is used in a time-dependent ionosphere model to calculate the response of the electron and ion density profiles. Then the spectral model is mathematically filtered to show how it would appear to the SOLRAD EUV detectors, and this degraded information is used in the ionosphere model. Comparison of the two ionosphere shows that the two spectra produces changes in the total electron content in the ionosphere that differ by only a few percent. More significant changes which occur in the individual species densities are described. Title: The detection of a companion star to the Cepheid variable T Monocerotis Authors: Mariska, J. T.; Doschek, G. A.; Feldman, U. Bibcode: 1980ApJ...242.1083M Altcode: We have obtained ultraviolet spectra with the International Ultraviolet Explorer (IUE) spacecraft of the classical Cepheid T Mon at several phases in the 27 day period. Significant ultraviolet emission is detected at wavelengths less than 1600 A, where little flux is expected from classical Cepheids. Furthermore, the emission at wavelengths less than about 1900 A does not vary with phase. Comparison with model atmosphere flux distributions shows that the emission is consistent with the flux expected from a companion star with an effective temperature of about 10,000 K (approximately A0) near the main sequence. Title: High-resolution X-ray spectra of solar flares. IV - General spectral properties of M type flares Authors: Feldman, U.; Doschek, G. A.; Kreplin, R. W.; Mariska, J. T. Bibcode: 1980ApJ...241.1175F Altcode: The spectral characteristics in selected narrow regions of the X-ray spectrum of class M solar flares are analyzed. High-resolution spectra in the ranges 1.82-1.97, 2.98-3.07, 3.14-3.24 and 8.26-8.53 A, which contain lines important for the determination of electron temperature and departure from ionization equilibrium, were recorded by spaceborne Bragg crystal spectrometers. Temperatures of up to 20,000,000 K are obtained from line ratios during flare rise phases in M as well as X flares, while in the decay phase the calcium temperature can be as low as 8,000,000 K, which is significantly lower than in X flares. Large nonthermal motions (on the order of 130 km/sec at most) are also observed in M as well as X flares, which are largest during the soft X-ray rise phase. Finally, it is shown that the method proposed by Gabriel and Phillips (1979) for detecting departures of electrons from Maxwellian velocity distributions is not sufficiently sensitive to give reliable results for the present data. Title: Numerical Simulation of a Cooling Flare Loop for Application to X-Ray Flare Spectra Authors: Doschek, G. A.; Boris, J. P.; Mariska, J. T.; Oran, E. S. Bibcode: 1980BAAS...12..912D Altcode: No abstract at ADS Title: A Dynamic Flux-Tube Model for Compressible MHD Processes in the Solar Atmosphere Authors: Boris, J. P.; Mariska, J. T.; Book, D. L.; Oran, E. S.; Young, T.; Doschek, G. A. Bibcode: 1980BAAS...12..908B Altcode: No abstract at ADS Title: Condensational Instability in Coronal Plasmas Authors: Oran, E. S.; Boris, J. P.; Mariska, J. T.; Doschek, G. A. Bibcode: 1980BAAS...12..910O Altcode: No abstract at ADS Title: Some Aspects of Transition Zone Dynamics Authors: Mariska, J. T.; Boris, J. P.; Oran, E. S.; Doschek, G. A. Bibcode: 1980BAAS...12..908M Altcode: No abstract at ADS Title: Physical conditions in the solar atmosphere above an active region Authors: Mariska, J. T.; Feldman, U.; Doschek, G. A. Bibcode: 1980ApJ...240..300M Altcode: From a series of EUV spectra obtained at several heights above the limb in a solar active region, the volume emission measure is derived as a function of the electron temperature in the temperature range 70,000-1,500,000 K and the electron density at two locations. The emission measure from the coronal material (temperature greater than 700,000 K) is nearly the same everywhere and represents most of the material in the line of sight, while the emission measure from the transition region material (temperature between 70,000 and 250,000 K) fluctuates by two orders of magnitude from position to position above the active region. This is in agreement with the picture of this active region as consisting of a number of well-defined loops or lower portions of loops at transition region temperatures that are inhomogeneously distributed in much larger and more diffuse loop structures at coronal temperatures. The coronal data are in reasonable agreement with simple coronal models. Emission measures near 1,000,000 K evaluated using different ions differ by a factor of 4, suggesting difficulties with the atomic physics data. Title: The detection of a companion star to the Cepheid variable eta Aql. Authors: Mariska, J. T.; Doschek, G. A.; Feldman, U. Bibcode: 1980ApJ...238L..87M Altcode: Ultraviolet spectra have been obtained with IUE of the classical Cepheid Eta Aquilae at several phases in the 7.18 day period. Significant ultraviolet emission is detected at wavelengths less than 1600 A, where little flux is expected from classical Cepheids. Furthermore, the emission at wavelengths less than about 1600 A does not vary with phase. Comparison with model atmosphere flux distributions shows that the nonvariable emission is consistent with the flux expected from a main-sequence companion star with an effective temperature of about 9500 K (A0 V). The observed ultraviolet flux and spectral type are used to compute a distance of 300 pc to the system, in agreement with the distance predicted using the period luminosity relation. Title: The Companion of Eta-Aquilae Authors: Mariska, J. T. Bibcode: 1980S&T....59..295M Altcode: No abstract at ADS Title: Mass Motions in the Transition Zone of Coronal Holes Authors: Doschek, G. A.; Mariska, J. T.; Feldman, U. Bibcode: 1980BAAS...12S.518D Altcode: No abstract at ADS Title: The Detection of an Early Type Companion Star to the Classical Cepheid T Mon Authors: Mariska, J. T.; Doschek, G. A.; Feldman, U. Bibcode: 1980BAAS...12Q.462M Altcode: No abstract at ADS Title: Relative chemical abundances in different solar regions Authors: Mariska, J. T. Bibcode: 1980ApJ...235..268M Altcode: Intensities of extreme-ultraviolet emission lines formed in quiet sun regions, a coronal hole, an active region, and a prominence are used to derive chemical abundances of carbon, nitrogen, and oxygen relative to silicon in each region. For each element the relative abundance in each region agrees to within the estimated errors in the analysis. This means that the relative abundances are constant over a wide range of electron densities, emission measures, turbulent mass motions, and heights above the limb. Uncertainties in the atomic data appear to be the primary source of scatter in the derived abundances. Title: The Detection of a Companion Star to the Cepheid Variable Eta Aquilae Authors: Mariska, J. T.; Doschek, G. A.; Feldman, U. Bibcode: 1979BAAS...11..687M Altcode: No abstract at ADS Title: Extreme-ultraviolet limb spectra of a prominence observed from Skylab. Authors: Mariska, J. T.; Doschek, G. A.; Feldman, U. Bibcode: 1979ApJ...232..929M Altcode: Line profiles of extreme ultraviolet emission lines observed in a solar prominence at positions above the white-light limb with the NRL slit spectrograph on Skylab are discussed. Absolute line intensities and full widths at half-maximum are presented, and emission measures, electron densities, and mass motions are derived at several locations within the prominence. For electron temperatures less than 40,000 K, the calculated mass motions are found to be near zero, while for electron temperatures greater than 40,000 K, the nonthermal velocity decreases with increasing height in the prominence. It is suggested that falling material is responsible for the fact that the measured electron density decreases with height less rapidly than the decrease predicted for a hydrostatic gas. In addition, from the He II 1640 A line profile, an average temperature of 27,000 K is derived for the region in which He II is emitted. Title: On the structure of the solar transition zone and lower corona. Authors: Feldman, U.; Doschek, G. A.; Mariska, J. T. Bibcode: 1979ApJ...229..369F Altcode: Recent observations of the solar transition zone and corona obtained primarily from NRL spectrographs on Skylab are summarized and used to examine the structure of the transition zone. The transition zone is revealed to be more inhomogeneous than is apparent from spectroheliograms with spatial resolution of about 3 arcsec. Transition-zone emission appears to arise in spicularlike structures. The effective area covered by the emitting structures at lower transition-zone temperatures (about 100,000 K) is only about 1% of the total surface area of the sun. The transition zone is highly inhomogeneous even over cell interior regions, where fluctuations in brightness by factors of 25 can occur. It is shown that homogeneous coronal models are not valid for the inner corona. Most of the higher-density inner corona is concentrated into looplike structures that extend down to the white-light limb. These structures are unrelated to the spicular-type structures that produce most of the transition-zone emission. Title: Relative Chemical Abundances in Different Solar Regions Authors: Mariska, J. T. Bibcode: 1979BAAS...11Q.405M Altcode: No abstract at ADS Title: Nonthermal broadening of extreme ultraviolet emission lines near the solar limb. Authors: Mariska, J. T.; Feldman, U.; Doschek, G. A. Bibcode: 1979A&A....73..361M Altcode: Summary. Line profiles of optically thin extreme ultraviolet emission lines observed in quiet-Sun regions at 8', 12', and 20' above the white light limb with the NRL slit spectrograph (5082-B) on Skylab are discussed. Random mass-motion velocities are calculated. The velocity is found to increase with increasing height above the white light limb for all the lines regardless of the temperature of formation between 4 l0 K and 2l0 K. At +12' a typical velocity is about 33km -1 Key words: Sun - transition zone - EUV spectra Title: Electron densities in the solar corona from density-sensitive line ratios in the N I isoelectronic sequence. Authors: Feldman, U.; Doschek, G. A.; Mariska, J. T.; Bhatia, A. K.; Mason, H. E. Bibcode: 1978ApJ...226..674F Altcode: Electron densities are derived in the solar inner corona from forbidden lines of S x near 1100 A. The density-sensitive line ratio considered is (4S0312-2D0312)/(4S0312-2D0612). The ratio is calculated as a function of density for four ions of the N I isoelectronic sequence, i.e., Mg VI, Si VIII, S x, and Ar XII. The variation of the ratio (4S0312-2P0312)/(4S0312-2D0312) with density is also calculated. The results are applied to off-limb spectra recorded by the NRL Skylab spectrograph. Densities were found to be the same in five quiet Sun regions and four active regions observed at heights > 8" outside the white-light limb. The average density derived from the S x lines for all regions considered is 1.0 x 10 cm -3. This result applies to plasma at the temperature of formation of S x, i.e., 1.3 x 106 K. At heights greater than 20" outside the limb the average density is 7.7 x 108 cm -3, and between 8" and 12" above the limb the average density is 1.0 x 10 cm 3, for both quiet Sun and active regions. Subject heading: Sun: corona Title: Measurements of extreme-ultraviolet emission-line profiles near the solar limb. Authors: Mariska, J. T.; Feldman, U.; Doschek, G. A. Bibcode: 1978ApJ...226..698M Altcode: Line profiles of optically thin extreme-ultraviolet emission lines observed in a quiet sun region at positions within and above the white-light limb with the NRL slit spectrograph (S082-B) on Skylab are discussed. Absolute line intensities and full widths at half-maximum are presented for lines formed over the temperature range from about 10,000 to 22,000 K. The line intensities are compared with the predictions of simple atmospheric models consisting of a spicule component and a thin spherically symmetric or network models, but can be explained by assuming that the emission arises from spicule-like inhomogeneities. Random mass-motion velocities are calculated. The velocity increases with increasing temperature of line formation. Near the limb and above about 4000 K the calculated velocity is consistent with the predictions of a constant acoustic flux passing through the transition zone. For the ions formed at temperatures not less than about 63,000 K, the velocity is found to increase with increasing height above the white-light limb. Title: Electron densities in stellar atmospheres determined from IUE spectra. Authors: Doschek, G. A.; Feldman, U.; Mariska, J. T.; Linsky, J. L. Bibcode: 1978ApJ...226L..35D Altcode: No abstract at ADS Title: Temperature gradients in the inner corona. Authors: Mariska, J. T.; Withbroe, G. L. Bibcode: 1978SoPh...60...67M Altcode: Emission gradient curves for extreme ultraviolet (EUV) resonance lines of O VI and Mg X have been constructed from spectroheliograms of quiet limb regions observed with the Harvard experiment on Skylab. An analysis of these data suggests that the coronal temperature rises throughout the height range 1.03R≤r≤1.3R. This result implies that in quiet regions there is significant coronal heating beyond r = 1.3R. Title: Analysis of extreme-ultraviolet observations of a polar coronal hole. Authors: Mariska, J. T. Bibcode: 1978ApJ...225..252M Altcode: Emission gradient curves for extreme-ultraviolet resonance lines of lithiumlike ions have been constructed from spectroheliograms of a northern polar coronal hole observed on August 14, 1973, with the Harvard experiment on Skylab. An emission-measure analysis indicates both reduced density and coronal temperature in the coronal hole. The boundary geometry of the coronal hole is determined, and a temperature-density model that is consistent with the observed intensities is constructed. The model gives a conductive flux of 60,000 erg/sq cm per sec at 1.03 solar radii. The boundary geometry and density distribution are combined with typical solar-wind parameters at the earth to determine an outflow velocity of 15 km/s at 1.08 solar radii. Title: A search for stellar oscillations. Authors: Traub, W. A.; Mariska, J. T.; Carleton, N. P. Bibcode: 1978ApJ...223..583T Altcode: A PEPSIOS spectrometer has been used to search for stellar photospheric oscillations with periods in the range from about 10 to 5000 s, and with velocity sensitivities down to about 1 m/s (rms) at the 1-sigma level. In the nine stars observed, no evidence is found for ocillations at the 3-sigma level. However, by using the same technique on the sun, the well-known 300-s oscillation was detected with an rms amplitude of 1.6 + or - 0.5 m/s for the integrated disk. Title: Nonthermal Broadening of Extreme Ultraviolet Emission Lines near the Solar Limb Authors: Mariska, J. T.; Feldman, U.; Doschek, G. A. Bibcode: 1978BAAS...10..432M Altcode: No abstract at ADS Title: A Composite Coronal Hole Model. Authors: Munro, R. H.; Mariska, J. T. Bibcode: 1977BAAS....9..370M Altcode: No abstract at ADS Title: The structure of the solar transition region and inner corona Authors: Mariska, John Thomas Bibcode: 1977PhDT.......265M Altcode: No abstract at ADS Title: The Structure of the Solar Transition Region and Inner Corona. Authors: Mariska, J. T. Bibcode: 1977PhDT........14M Altcode: Emission gradient curves for extreme ultraviolet resonance lines of lithium-like ions were constructed from spectroheliograms of quiet limb regions and a north polar coronal hole observed with the Harvard experiment on Skylab. The observations are interpreted with simple coronal models. The coronal models are extended downward and the calculated emission from them is compared with averaged, network and cell line intensities to derive models in a quiet region and a coronal hole. The energy balance implications of the models are examined. In the transition region both conduction and radiation are important in determining the energy balance in network regions in both quiet areas and coronal holes. Additional energy sources are required in the network in coronal holes. In the corona, the energy losses, and hence the requirements for mechanical heating, are the same in quiet regions and coronal holes. Title: Analysis of EUV limb brightening observations from ATM. II: Influence of spicules. Authors: Withbroe, G. L.; Mariska, J. T. Bibcode: 1976SoPh...48...21W Altcode: A comparison of limb brightening measurements with theoretical limb brightening curves calculated for simple atmospheric models indicates that a significant fraction of the EUV emission from lines formed in the transition layer comes from spicules. We find that spicules contribute about 20% of the total quiet Sun intensity for lines of the C II, C III, N III, and O VI ions. The uncertainty in the magnitude of the percentage is about a factor of 2. The EUV-emission scale heights above the limb are consistent with the assumption that the variation with height of the number of EUV-emitting spicules is the same as for Hα-emitting spicules. Optical depths derived for the C II λ1335 and C III λ977 lines yield estimates for the pressure P = neT in the transition layer, log P = 14.7±0.5, that are in good agreement with pressures derived under the assumption that the transition layer is in pressure equilibrium with the chromosphere and corona. Title: Extreme Ultraviolet Observations of a Polar Coronal Hole Authors: Mariska, J. T. Bibcode: 1976BAAS....8R.338M Altcode: No abstract at ADS Title: Analysis of EUV Limb-Brightening Observations from ATM. I: Model for the Transition Layer and the Corona Authors: Mariska, J. T.; Withbroe, G. L. Bibcode: 1975SoPh...44...55M Altcode: Limb-brightening curves for EUV resonance lines of O VI and Mg X have been constructed from spectroheliograms (5″ resolution) of quiet limb regions observed with the Harvard experiment on Skylab. The observations are interpreted with a simple model for the transition layer and the corona. A comparison of theoretical and observed limb-brightening curves indicates that the lower boundary of the corona, where Te= 106K, is at a height of about 8000 km in typical quiet areas. For 1.01 R≲r1.25 R, the corona can be represented by a homogeneous model in hydrostatic equilibrium with a temperature of 106K for 1.01 R≲r<1.1 R and 1.1 × 106K for r≳1.1 R. The model for the transition layer is inhomogeneous, with the temperature gradient a factor of 3 shallower in the network than in the intranetwork regions. It appears that spicules should be included in the model in order to account for the penetration into the corona of cool (Te<106K) EUV-emitting material to heights up to 20000 km above the limb. Title: Extreme Ultraviolet Solar Limb Brighteness Observations Authors: Mariska, J. T.; Withbroe, G. L. Bibcode: 1975BAAS....7Q.460M Altcode: No abstract at ADS Title: Extreme Ultraviolet Solar Limb Brightening Observations of Lithium-Like Ions Authors: Mariska, J. T.; Withbroe, G. L. Bibcode: 1975BAAS....7..354M Altcode: No abstract at ADS Title: Solar Activity and the Variations of the Geomagnetic Kp-Index. I: Photospheric Activity Authors: Mariska, John T.; Oster, Ludwig Bibcode: 1972SoPh...26..241M Altcode: A careful correlation analysis is made between various types of solar activity as observed at photospheric levels and the daily variations of the geomagnetic Kp-index which, in turn, is a measure of the solar wind speed. We find that in no case does a significant enough correlation exist to pin-point a physical relation between some aspect of photospheric activity and the solar wind speed. It is concluded that the physical processes that do determine the wind speed occur at coronal heights. Title: Solar Activity and the Variation of the Geomagnetic Kp-Index Authors: Oster, Ludwig; Mariska, John T.; Altschuler, Martin D.; Trotter, Dorothy E. Bibcode: 1972BAAS....4R.389O Altcode: No abstract at ADS Title: Equilibrium, Pulsational, and Secular Stability Properties of the Lower Carbon-Burning Main Sequence Authors: Mariska, John T.; Hansen, Carl J. Bibcode: 1972ApJ...171..317M Altcode: Results are presented for stellar models composed of equal amounts of 12C and 100 in complete equilibrium within the mass range 0.82 < M/M0 < 2.31. The character of the static models is analogous to the lower helium main sequence in that they are double-valued with respect to mass whereas the central density is monotonic along the sequence. All the models are pulsationally unstable, but only one, near the minimum mass, is secularly unstable.