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Author name code: hayek
ADS astronomy entries on 2022-09-14
author:"Hayek, Wolfgang" 

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Title: The benchmark halo giant HD 122563: CNO abundances revisited
    with three-dimensional hydrodynamic model stellar atmospheres
Authors: Collet, R.; Nordlund, Å.; Asplund, M.; Hayek, W.;
   Trampedach, R.
2018MNRAS.475.3369C    Altcode: 2017arXiv171208099C
  We present an abundance analysis of the low-metallicity benchmark
  red giant star HD 122563 based on realistic, state-of-the-art,
  high-resolution, three-dimensional (3D) model stellar atmospheres
  including non-grey radiative transfer through opacity binning with
  4, 12, and 48 bins. The 48-bin 3D simulation reaches temperatures
  lower by ∼300-500 K than the corresponding 1D model in the upper
  atmosphere. Small variations in the opacity binning, adopted line
  opacities, or chemical mixture can cool the photospheric layers by
  a further ∼100-300 K and alter the effective temperature by ∼100
  K. A 3D local thermodynamic equilibrium (LTE) spectroscopic analysis
  of Fe I and Fe II lines gives discrepant results in terms of derived
  Fe abundance, which we ascribe to non-LTE effects and systematic errors
  on the stellar parameters. We also determine C, N, and O abundances by
  simultaneously fitting CH, OH, NH, and CN molecular bands and lines
  in the ultraviolet, visible, and infrared. We find a small positive
  3D-1D abundance correction for carbon (+0.03 dex) and negative ones for
  nitrogen (-0.07 dex) and oxygen (-0.34 dex). From the analysis of the [O
  I] line at 6300.3 Å, we derive a significantly higher oxygen abundance
  than from molecular lines (+0.46 dex in 3D and +0.15 dex in 1D). We rule
  out important OH photodissociation effects as possible explanation for
  the discrepancy and note that lowering the surface gravity would reduce
  the oxygen abundance difference between molecular and atomic indicators.

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Title: The elemental composition of the Sun. I. The intermediate
    mass elements Na to Ca
Authors: Scott, Pat; Grevesse, Nicolas; Asplund, Martin; Sauval,
   A. Jacques; Lind, Karin; Takeda, Yoichi; Collet, Remo; Trampedach,
   Regner; Hayek, Wolfgang
2015A&A...573A..25S    Altcode: 2014arXiv1405.0279S
  The chemical composition of the Sun is an essential piece of reference
  data for astronomy, cosmology, astroparticle, space and geo-physics:
  elemental abundances of essentially all astronomical objects are
  referenced to the solar composition, and basically every process
  involving the Sun depends on its composition. This article, dealing
  with the intermediate-mass elements Na to Ca, is the first in a
  series describing the comprehensive re-determination of the solar
  composition. In this series we severely scrutinise all ingredients
  of the analysis across all elements, to obtain the most accurate,
  homogeneous and reliable results possible. We employ a highly
  realistic 3D hydrodynamic model of the solar photosphere, which has
  successfully passed an arsenal of observational diagnostics. For
  comparison, and to quantify remaining systematic errors, we repeat
  the analysis using three different 1D hydrostatic model atmospheres
  (marcs, miss and Holweger & Müller 1974, Sol. Phys., 39, 19) and
  a horizontally and temporally-averaged version of the 3D model (⟨ 3D
  ⟩). We account for departures from local thermodynamic equilibrium
  (LTE) wherever possible. We have scoured the literature for the best
  possible input data, carefully assessing transition probabilities,
  hyperfine splitting, partition functions and other data for inclusion
  in the analysis. We have put the lines we use through a very stringent
  quality check in terms of their observed profiles and atomic data, and
  discarded all that we suspect to be blended. Our final recommended
  3D+NLTE abundances are: log ɛ<SUB>Na</SUB> = 6.21 ± 0.04, log
  ɛ<SUB>Mg</SUB> = 7.59 ± 0.04, log ɛ<SUB>Al</SUB> = 6.43 ± 0.04,
  log ɛ<SUB>Si</SUB> = 7.51 ± 0.03, log ɛ<SUB>P</SUB> = 5.41 ± 0.03,
  log ɛ<SUB>S</SUB> = 7.13 ± 0.03, log ɛ<SUB>K</SUB> = 5.04 ± 0.05
  and log ɛ<SUB>Ca</SUB> = 6.32 ± 0.03. The uncertainties include both
  statistical and systematic errors. Our results are systematically
  smaller than most previous ones with the 1D semi-empirical
  Holweger &amp; Müller model, whereas the ⟨ 3D ⟩ model returns
  abundances very similar to the full 3D calculations. This analysis
  provides a complete description and a slight update of the results
  presented in Asplund et al. (2009, ARA&amp;A, 47, 481) for Na to
  Ca, and includes full details of all lines and input data used. <P
  />Tables 1-4 and Appendix A are available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201424109/olm">http://www.aanda.org</A>

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Title: Accuracy tests of radiation schemes used in hot Jupiter global
    circulation models
Authors: Amundsen, David S.; Baraffe, Isabelle; Tremblin, Pascal;
   Manners, James; Hayek, Wolfgang; Mayne, Nathan J.; Acreman, David M.
2014A&A...564A..59A    Altcode: 2014arXiv1402.0814S
  The treatment of radiation transport in global circulation models (GCMs)
  is crucial for correctly describing Earth and exoplanet atmospheric
  dynamics processes. The two-stream approximation and correlated-k
  method are currently state-of-the-art approximations applied in both
  Earth and hot Jupiter GCM radiation schemes to facilitate the rapid
  calculation of fluxes and heating rates. Their accuracy have been
  tested extensively for Earth-like conditions, but verification of the
  methods' applicability to hot Jupiter-like conditions is lacking in
  the literature. We are adapting the UK Met Office GCM, the Unified
  Model (UM), for the study of hot Jupiters, and present in this work
  the adaptation of the Edwards-Slingo radiation scheme based on the
  two-stream approximation and the correlated-k method. We discuss the
  calculation of absorption coefficients from high-temperature line
  lists and highlight the large uncertainty in the pressure-broadened
  line widths. We compare fluxes and heating rates obtained with our
  adapted scheme to more accurate discrete ordinate (DO) line-by-line
  (LbL) calculations ignoring scattering effects. We find that, in
  most cases, errors stay below 10% for both heating rates and fluxes
  using ~10 k-coefficients in each band and a diffusivity factor D =
  1.66. The two-stream approximation and the correlated-k method both
  contribute non-negligibly to the total error. We also find that using
  band-averaged absorption coefficients, which have previously been used
  in radiative-hydrodynamical simulations of a hot Jupiter, may yield
  errors of ~100%, and should thus be used with caution.

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Title: The Stagger-grid: A grid of 3D stellar atmosphere
    models. II. Horizontal and temporal averaging and spectral line
    formation
Authors: Magic, Z.; Collet, R.; Hayek, W.; Asplund, M.
2013A&A...560A...8M    Altcode: 2013arXiv1307.3273M
  <BR /> Aims: We study the implications of averaging methods with
  different reference depth scales for 3D hydrodynamical model atmospheres
  computed with the Stagger-code. The temporally and spatially averaged
  (hereafter denoted as ⟨3D⟩) models are explored in the light
  of local thermodynamic equilibrium (LTE) spectral line formation by
  comparing spectrum calculations using full 3D atmosphere structures
  with those from ⟨3D⟩ averages. <BR /> Methods: We explored methods
  for computing mean ⟨3D⟩ stratifications from the Stagger-grid
  time-dependent 3D radiative hydrodynamical atmosphere models by
  considering four different reference depth scales (geometrical depth,
  column-mass density, and two optical depth scales). Furthermore,
  we investigated the influence of alternative averages (logarithmic,
  enforced hydrostatic equilibrium, flux-weighted temperatures). For the
  line formation we computed curves of growth for Fe i and Fe ii lines in
  LTE. <BR /> Results: The resulting ⟨3D⟩ stratifications for the four
  reference depth scales can be very different. We typically find that in
  the upper atmosphere and in the superadiabatic region just below the
  optical surface, where the temperature and density fluctuations are
  highest, the differences become considerable and increase for higher
  T<SUB>eff</SUB>, lower log g, and lower [Fe / H]. The differential
  comparison of spectral line formation shows distinctive differences
  depending on which ⟨3D⟩ model is applied. The averages over
  layers of constant column-mass density yield the best mean ⟨3D⟩
  representation of the full 3D models for LTE line formation, while
  the averages on layers at constant geometrical height are the least
  appropriate. Unexpectedly, the usually preferred averages over layers of
  constant optical depth are prone to increasing interference by reversed
  granulation towards higher effective temperature, in particular at
  low metallicity. <P />Appendix A is available in electronic form
  at <A href="http://www.aanda.org">http://www.aanda.org</A>Mean
  ⟨3D⟩ models are available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr">http://cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/560/A8">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/560/A8</A>
  as well as at <A
  href="http://www.stagger-stars.net">http://www.stagger-stars.net</A>

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Title: VizieR Online Data Catalog: STAGGER-grid of 3D stellar
    models. II. (Magic+, 2013)
Authors: Magic, Z.; Collet, R.; Hayek, W.; Asplund, M.
2013yCat..35600008M    Altcode: 2013yCat..35609008M
  More (updated) information and data available at:
  http://www.stagger-stars.net/ <P />(5 data files).

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Title: The Stagger-grid: A grid of 3D stellar atmosphere
    models. I. Methods and general properties
Authors: Magic, Z.; Collet, R.; Asplund, M.; Trampedach, R.; Hayek,
   W.; Chiavassa, A.; Stein, R. F.; Nordlund, Å.
2013A&A...557A..26M    Altcode: 2013arXiv1302.2621M
  <BR /> Aims: We present the Stagger-grid, a comprehensive grid of
  time-dependent, three-dimensional (3D), hydrodynamic model atmospheres
  for late-type stars with realistic treatment of radiative transfer,
  covering a wide range in stellar parameters. This grid of 3D models is
  intended for various applications besides studies of stellar convection
  and atmospheres per se, including stellar parameter determination,
  stellar spectroscopy and abundance analysis, asteroseismology,
  calibration of stellar evolution models, interferometry, and extrasolar
  planet search. In this introductory paper, we describe the methods
  we applied for the computation of the grid and discuss the general
  properties of the 3D models as well as of their temporal and spatial
  averages (here denoted ⟨3D⟩ models). <BR /> Methods: All our models
  were generated with the Stagger-code, using realistic input physics for
  the equation of state (EOS) and for continuous and line opacities. Our ~
  220 grid models range in effective temperature, T<SUB>eff</SUB>, from
  4000 to 7000 K in steps of 500 K, in surface gravity, log g, from 1.5
  to 5.0 in steps of 0.5 dex, and metallicity, [Fe/H], from - 4.0 to +
  0.5 in steps of 0.5 and 1.0 dex. <BR /> Results: We find a tight scaling
  relation between the vertical velocity and the surface entropy jump,
  which itself correlates with the constant entropy value of the adiabatic
  convection zone. The range in intensity contrast is enhanced at lower
  metallicity. The granule size correlates closely with the pressure
  scale height sampled at the depth of maximum velocity. We compare the
  ⟨3D⟩ models with currently widely applied one-dimensional (1D)
  atmosphere models, as well as with theoretical 1D hydrostatic models
  generated with the same EOS and opacity tables as the 3D models, in
  order to isolate the effects of using self-consistent and hydrodynamic
  modeling of convection, rather than the classical mixing length theory
  approach. For the first time, we are able to quantify systematically
  over a broad range of stellar parameters the uncertainties of 1D
  models arising from the simplified treatment of physics, in particular
  convective energy transport. In agreement with previous findings,
  we find that the differences can be rather significant, especially
  for metal-poor stars. <P />Appendices A-C are available in electronic
  form at <A href="http://www.aanda.org">http://www.aanda.org</A>Full
  Table C.1 is available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr">http://cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/557/A26">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/557/A26</A>

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Title: VizieR Online Data Catalog: STAGGER-grid of 3D stellar
    models. I. (Magic+, 2013)
Authors: Magic, Z.; Collet, R.; Asplund, M.; Trampedach, R.; Hayek,
   W.; Chiavassa, A.; Stein, R. F.; Nordlund, A.
2013yCat..35570026M    Altcode: 2013yCat..35579026M
  The 3D model atmospheres presented here were constructed with
  a custom version of the Stagger-code, a state-of-the-art,
  multipurpose, radiative-magnetohydrodynamics (R-MHD)
  code originally developed by Nordlund &amp; Galsgaard (1995,
  http://www.astro.ku.dk/~kg/Papers/MHD_code.ps.gz), and continuously
  improved over the years by its user community. <P />(1 data file).

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Title: Limb darkening laws for two exoplanet host stars derived
    from 3D stellar model atmospheres. Comparison with 1D models and
    HST light curve observations
Authors: Hayek, W.; Sing, D.; Pont, F.; Asplund, M.
2012A&A...539A.102H    Altcode: 2012arXiv1202.0548H
  We compare limb darkening laws derived from 3D hydrodynamical model
  atmospheres and 1D hydrostatic MARCS models for the host stars of
  two well-studied transiting exoplanet systems, the late-type dwarfs
  <ASTROBJ>HD 209458</ASTROBJ> and <ASTROBJ>HD 189733</ASTROBJ>. The
  surface brightness distribution of the stellar disks is calculated
  for a wide spectral range using 3D LTE spectrum formation and opacity
  sampling<SUP>⋆</SUP>. We test our theoretical predictions using
  least-squares fits of model light curves to wavelength-integrated
  primary eclipses that were observed with the Hubble Space Telescope
  (HST). The limb darkening law derived from the 3D model of HD 209458 in
  the spectral region between 2900 Å and 5700 Å produces significantly
  better fits to the HST data, removing systematic residuals that were
  previously observed for model light curves based on 1D limb darkening
  predictions. This difference arises mainly from the shallower mean
  temperature structure of the 3D model, which is a consequence of the
  explicit simulation of stellar surface granulation where 1D models
  need to rely on simplified recipes. In the case of HD 189733, the
  model atmospheres produce practically equivalent limb darkening curves
  between 2900 Å and 5700 Å, partly due to obstruction by spectral
  lines, and the data are not sufficient to distinguish between the
  light curves. We also analyze HST observations between 5350 Å and
  10 500 Å for this star; the 3D model leads to a better fit compared
  to 1D limb darkening predictions. The significant improvement of fit
  quality for the HD 209458 system demonstrates the higher degree of
  realism of 3D hydrodynamical models and the importance of surface
  granulation for the formation of the atmospheric radiation field of
  late-type stars. This result agrees well with recent investigations of
  limb darkening in the solar continuum and other observational tests of
  the 3D models. The case of HD 189733 is no contradiction as the model
  light curves are less sensitive to the temperature stratification
  of the stellar atmosphere and the observed data in the 2900-5700
  Å region are not sufficient to distinguish more clearly between
  the 3D and 1D limb darkening predictions. <P />Full theoretical
  spectra for both stars are available in electronic form at the
  CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/539/A102">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/539/A102</A>,
  as well as at <A
  href="http://www.astro.ex.ac.uk/people/sing">www.astro.ex.ac.uk/people/sing</A>.

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Title: Simulations of the solar near-surface layers with the CO5BOLD,
    MURaM, and Stagger codes
Authors: Beeck, B.; Collet, R.; Steffen, M.; Asplund, M.; Cameron,
   R. H.; Freytag, B.; Hayek, W.; Ludwig, H. -G.; Schüssler, M.
2012A&A...539A.121B    Altcode: 2012arXiv1201.1103B
  Context. Radiative hydrodynamic simulations of solar and stellar surface
  convection have become an important tool for exploring the structure and
  gas dynamics in the envelopes and atmospheres of late-type stars and for
  improving our understanding of the formation of stellar spectra. <BR
  /> Aims: We quantitatively compare results from three-dimensional,
  radiative hydrodynamic simulations of convection near the solar surface
  generated with three numerical codes (CO<SUP>5</SUP>BOLD, MURaM,
  and Stagger) and different simulation setups in order to investigate
  the level of similarity and to cross-validate the simulations. <BR
  /> Methods: For all three simulations, we considered the average
  stratifications of various quantities (temperature, pressure, flow
  velocity, etc.) on surfaces of constant geometrical or optical depth,
  as well as their temporal and spatial fluctuations. We also compared
  observables, such as the spatially resolved patterns of the emerging
  intensity and of the vertical velocity at the solar optical surface
  as well as the center-to-limb variation of the continuum intensity
  at various wavelengths. <BR /> Results: The depth profiles of the
  thermodynamical quantities and of the convective velocities as well as
  their spatial fluctuations agree quite well. Slight deviations can be
  understood in terms of differences in box size, spatial resolution
  and in the treatment of non-gray radiative transfer between the
  simulations. <BR /> Conclusions: The results give confidence in the
  reliability of the results from comprehensive radiative hydrodynamic
  simulations.

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Title: VizieR Online Data Catalog: HD 209458 and HD 189733 theoretical
    spectra (Hayek+, 2012)
Authors: Hayek, W.; Sing, D.; Pont, F.; Asplund, M.
2012yCat..35390102H    Altcode: 2012yCat..35399102H
  Theoretical spectrum computations for the G-type dwarf HD 209458 and
  the K-type dwarf HD 189733 are presented, based on 3D hydrodynamical
  models of the stellar atmospheres. Surface intensities were computed
  in LTE using the SCATE spectrum formation code and cover the wavelength
  region between about 910 Angstroem and 20 micron with constant sampling
  of R=λ/δ_λ=20,000. The stellar disk was sampled at the disk center
  (μ=cos(θ)=1.0) and at angles μ = 0.90, 0.80, 0.70, 0.60, 0.50,
  0.40, 0.30, 0.25, 0.20, 0.15, 0.125, 0.1, 0.075, 0.05, 0.025, 0.01
  towards the limb. Use integration weights 0.05, 0.1, 0.1, 0.1, 0.1,
  0.1, 0.1, 0.075, 0.05, 0.05, 0.0375, 0.025, 0.025, 0.025, 0.025, 0.02,
  0.0125 to obtain fluxes. <P />(2 data files).

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Title: On the effects of clouds and hazes in the atmospheres of hot
Jupiters: semi-analytical temperature-pressure profiles
Authors: Heng, Kevin; Hayek, Wolfgang; Pont, Frédéric; Sing, David K.
2012MNRAS.420...20H    Altcode: 2011MNRAS.tmp.2117H; 2011arXiv1107.1390H
  Motivated by the work of Guillot, we present a semi-analytical
  formalism for calculating the temperature-pressure profiles in hot
  Jovian atmospheres which includes the effects of clouds/hazes and
  collision-induced absorption. Using the dual-band approximation,
  we assume that stellar irradiation and thermal emission from the
  hot Jupiter occur at distinct wavelengths ('shortwave' versus
  'longwave'). For a purely absorbing cloud/haze, we demonstrate its
  dual effect of cooling and warming the upper and lower atmosphere,
  respectively, which modifies, in a non-trivial manner, the condition for
  whether a temperature inversion is present in the upper atmosphere. The
  warming effect becomes more pronounced as the cloud/haze deck resides at
  greater depths. If it sits below the shortwave photosphere, the warming
  effect becomes either more subdued or ceases altogether. If shortwave
  scattering is present, its dual effect is to warm and cool the upper
  and lower atmospheres, respectively, thus counteracting the effects
  of enhanced longwave absorption by the cloud/haze. We make a tentative
  comparison of a four-parameter model to the temperature-pressure data
  points inferred from the observations of HD 189733b and estimate that
  its Bond albedo is approximately 10 per cent. Besides their utility
  in developing physical intuition, our semi-analytical models are a
  guide for the parameter space exploration of hot Jovian atmospheres
  via three-dimensional simulations of atmospheric circulation.

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Title: Effects of Scattering on the Temperature Stratification in
    3D Model Atmospheres of Late-Type Stars
Authors: Collet, R.; Hayek, W.; Asplund, M.
2011ASPC..448..819C    Altcode: 2011csss...16..819C
  Three-dimensional (3D) radiative hydrodynamic model atmospheres
  of metal-poor late-type stars predict cooler upper photospheric
  stratifications than their one-dimensional (1D) counterparts. This
  property of 3D model atmospheres affects the determination of
  elemental abundances from temperature-sensitive spectral features, with
  important consequences for galactic chemical evolution studies. In this
  contribution, we investigate the impact of different approximations
  of scattering in the solution of the radiative transfer equation on
  the temperature stratification of 3D model atmospheres of metal-poor
  red giants. We use the BIFROST code to construct 3D model atmospheres
  of metal-poor red giants using three different approximations of
  scattering. First, we self-consistently solve the radiative transfer
  equation for the general case of a source function with a coherent
  scattering term; second, we solve the radiative transfer equation
  assuming a Planckian source function and neglecting altogether
  the contribution of continuum scattering to extinction in the
  optically thin layers; third, we assume a Planckian source function
  and treat continuum scattering as pure absorption everywhere in the
  simulation's domain. We find that the second approach produces very
  similar temperature structures with cool upper photospheric layers as
  when treating scattering correctly, and at a much lower computational
  cost. In contrast, treating scattering as pure absorption leads to
  significantly hotter and shallower temperature stratifications.

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Title: Hubble Space Telescope transmission spectroscopy of the
exoplanet HD 189733b: high-altitude atmospheric haze in the optical
    and near-ultraviolet with STIS
Authors: Sing, D. K.; Pont, F.; Aigrain, S.; Charbonneau, D.; Désert,
   J. -M.; Gibson, N.; Gilliland, R.; Hayek, W.; Henry, G.; Knutson,
   H.; Lecavelier Des Etangs, A.; Mazeh, T.; Shporer, A.
2011MNRAS.416.1443S    Altcode: 2011arXiv1103.0026S; 2011MNRAS.tmp.1159S
  We present Hubble Space Telescope (HST) optical and near-ultraviolet
  transmission spectra of the transiting hot Jupiter HD 189733b,
  taken with the repaired Space Telescope Imaging Spectrograph (STIS)
  instrument. The resulting spectra cover the range 2900-5700 Å and reach
  per exposure signal-to-noise ratio levels greater than 11 000 within
  a 500-Å bandwidth. We used time series spectra obtained during two
  transit events to determine the wavelength dependence of the planetary
  radius and measure the exoplanet's atmospheric transmission spectrum
  for the first time over this wavelength range. Our measurements,
  in conjunction with existing HST spectra, now provide a broad-band
  transmission spectrum covering the full optical regime. The STIS
  data also show unambiguous evidence of a large occulted stellar spot
  during one of our transit events, which we use to place constraints on
  the characteristics of the K dwarf's stellar spots, estimating spot
  temperatures around T<SUB>eff</SUB>∼ 4250 K. With contemporaneous
  ground-based photometric monitoring of the stellar variability,
  we also measure the correlation between the stellar activity level
  and transit-measured planet-to-star radius contrast, which is in good
  agreement with predictions. We find a planetary transmission spectrum in
  good agreement with that of Rayleigh scattering from a high-altitude
  atmospheric haze as previously found from HST Advanced Camera for
  Surveys. The high-altitude haze is now found to cover the entire optical
  regime and is well characterized by Rayleigh scattering. These findings
  suggest that haze may be a globally dominant atmospheric feature of
  the planet which would result in a high optical albedo at shorter
  optical wavelengths.

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Title: The Effect of Scattering on the Temperature Stratification
    of 3D Model Atmospheres of Metal-Poor Red Giants
Authors: Collet, Remo; Hayek, Wolfgang; Asplund, Martin
2011IAUS..271..373C    Altcode:
  We study the effects of different approximations of scattering in 3D
  radiation-hydrodynamics simulations on the photospheric temperature
  stratification of metal-poor red giant stars. We find that assuming a
  Planckian source function and neglecting the contribution of scattering
  to extinction in optically thin layers provides a good approximation
  of the effects of coherent scattering on the photospheric temperature
  balance.

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Title: The stellar atmosphere simulation code Bifrost. Code
    description and validation
Authors: Gudiksen, B. V.; Carlsson, M.; Hansteen, V. H.; Hayek, W.;
   Leenaarts, J.; Martínez-Sykora, J.
2011A&A...531A.154G    Altcode: 2011arXiv1105.6306G
  Context. Numerical simulations of stellar convection and photospheres
  have been developed to the point where detailed shapes of observed
  spectral lines can be explained. Stellar atmospheres are very complex,
  and very different physical regimes are present in the convection zone,
  photosphere, chromosphere, transition region and corona. To understand
  the details of the atmosphere it is necessary to simulate the whole
  atmosphere since the different layers interact strongly. These physical
  regimes are very diverse and it takes a highly efficient massively
  parallel numerical code to solve the associated equations. <BR /> Aims:
  The design, implementation and validation of the massively parallel
  numerical code Bifrost for simulating stellar atmospheres from the
  convection zone to the corona. <BR /> Methods: The code is subjected
  to a number of validation tests, among them the Sod shock tube test,
  the Orzag-Tang colliding shock test, boundary condition tests and
  tests of how the code treats magnetic field advection, chromospheric
  radiation, radiative transfer in an isothermal scattering atmosphere,
  hydrogen ionization and thermal conduction. Results.Bifrost completes
  the tests with good results and shows near linear efficiency scaling
  to thousands of computing cores.

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Title: 3D LTE spectral line formation with scattering in red giant
    stars
Authors: Hayek, W.; Asplund, M.; Collet, R.; Nordlund, Å.
2011A&A...529A.158H    Altcode: 2011arXiv1108.3366H
  <BR /> Aims: We investigate the effects of coherent isotropic continuum
  scattering on the formation of spectral lines in local thermodynamic
  equilibrium (LTE) using 3D hydrodynamical and 1D hydrostatic model
  atmospheres of red giant stars. <BR /> Methods: Detailed radiative
  transfer with coherent and isotropic continuum scattering is computed
  for 3D hydrodynamical and 1D hydrostatic models of late-type stellar
  atmospheres using the SCATE code. Opacities are computed in LTE, while
  a coherent and isotropic scattering term is added to the continuum
  source function. We investigate the effects of scattering by comparing
  continuum flux levels, spectral line profiles and curves of growth
  for different species with calculations that treat scattering as
  absorption. <BR /> Results: Rayleigh scattering is the dominant source
  of scattering opacity in the continuum of red giant stars. Photons
  may escape from deeper, hotter layers through scattering, resulting in
  significantly higher continuum flux levels beneath a wavelength of λ
  ≲ 5000 Å. The magnitude of the effect is determined by the importance
  of scattering opacity with respect to absorption opacity; we observe
  the largest changes in continuum flux at the shortest wavelengths
  and lowest metallicities; intergranular lanes of 3D models are more
  strongly affected than granules. Continuum scattering acts to increase
  the profile depth of LTE lines: continua gain more brightness than line
  cores due to their larger thermalization depth in hotter layers. We
  thus observe the strongest changes in line depth for high-excitation
  species and ionized species, which contribute significantly to photon
  thermalization through their absorption opacity near the continuum
  optical surface. Scattering desaturates the line profiles, leading to
  larger abundance corrections for stronger lines, which reach -0.5 dex
  at 3000 Å for Fe ii lines in 3D with excitation potential χ = 2 eV at
  [Fe/H] = -3.0. The corrections are less severe for low-excitation lines,
  longer wavelengths, and higher metallicity. Velocity fields increase
  the effects of scattering by separating emission from granules and
  intergranular lanes in wavelength. 1D calculations exhibit similar
  scattering abundance corrections for weak lines, but those for
  strong lines are generally smaller compared to 3D models and depend
  on the choice of microturbulence. <BR /> Conclusions: Continuum
  scattering should be taken into account for computing realistic
  spectral line profiles at wavelengths λ ≲ 4000 Å in metal-poor
  giant stars. Profile shapes are strongly affected by velocity fields
  and horizontal inhomogeneities, requiring a treatment based on 3D
  hydrodynamical rather than classical 1D hydrostatic model atmospheres.

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Title: Three-dimensional surface convection simulations of metal-poor
    stars. The effect of scattering on the photospheric temperature
    stratification
Authors: Collet, R.; Hayek, W.; Asplund, M.; Nordlund, Å.; Trampedach,
   R.; Gudiksen, B.
2011A&A...528A..32C    Altcode: 2011arXiv1101.3265C
  Context. Three-dimensional (3D) radiative hydrodynamic model atmospheres
  of metal-poor late-type stars are characterized by cooler upper
  photospheric layers than their one-dimensional counterparts. This
  property of 3D model atmospheres can dramatically affect the
  determination of elemental abundances from temperature-sensitive
  spectral features, with profound consequences on galactic chemical
  evolution studies. <BR /> Aims: We investigate whether the cool surface
  temperatures predicted by 3D model atmospheres of metal-poor stars
  can be ascribed to approximations in the treatment of scattering
  during the modelling phase. <BR /> Methods: We use the Bifrost
  code to construct 3D model atmospheres of metal-poor stars and test
  three different ways to handle scattering in the radiative transfer
  equation. As a first approach, we solve iteratively the radiative
  transfer equation for the general case of a source function with
  a coherent scattering term, treating scattering in a correct and
  consistent way. As a second approach, we solve the radiative transfer
  equation in local thermodynamic equilibrium approximation, neglecting
  altogether the contribution of continuum scattering to extinction in the
  optically thin layers; this has been the default mode in our previous
  3D modelling as well as in present Stagger-Code models. As our third
  and final approach, we treat continuum scattering as pure absorption
  everywhere, which is the standard case in the 3D modelling by the
  CO<SUP>5</SUP>BOLD collaboration. <BR /> Results: For all simulations,
  we find that the second approach produces temperature structures
  with cool upper photospheric layers very similar to the case in which
  scattering is treated correctly. In contrast, treating scattering as
  pure absorption leads instead to significantly hotter and shallower
  temperature stratifications. The main differences in temperature
  structure between our published models computed with the Stagger-
  and Bifrost codes and those generated with the CO<SUP>5</SUP>BOLD
  code can be traced to the different treatments of scattering. <BR />
  Conclusions: Neglecting the contribution of continuum scattering to
  extinction in optically thin layers provides a good approximation
  to the full, iterative solution of the radiative transfer equation
  in metal-poor stellar surface convection simulations, and at a much
  lower computational cost. Our results also demonstrate that the cool
  temperature stratifications predicted for metal-poor late-type stars
  by previous models by our collaboration are not an artifact of the
  approximated treatment of scattering.

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Title: Radiative transfer with scattering for domain-decomposed 3D
    MHD simulations of cool stellar atmospheres. Numerical methods and
    application to the quiet, non-magnetic, surface of a solar-type star
Authors: Hayek, W.; Asplund, M.; Carlsson, M.; Trampedach, R.; Collet,
   R.; Gudiksen, B. V.; Hansteen, V. H.; Leenaarts, J.
2010A&A...517A..49H    Altcode: 2010arXiv1007.2760H
  <BR /> Aims: We present the implementation of a radiative
  transfer solver with coherent scattering in the new BIFROST
  code for radiative magneto-hydrodynamical (MHD) simulations of
  stellar surface convection. The code is fully parallelized using
  MPI domain decomposition, which allows for large grid sizes and
  improved resolution of hydrodynamical structures. We apply the code
  to simulate the surface granulation in a solar-type star, ignoring
  magnetic fields, and investigate the importance of coherent scattering
  for the atmospheric structure. <BR /> Methods: A scattering term
  is added to the radiative transfer equation, requiring an iterative
  computation of the radiation field. We use a short-characteristics-based
  Gauss-Seidel acceleration scheme to compute radiative flux divergences
  for the energy equation. The effects of coherent scattering are
  tested by comparing the temperature stratification of three 3D
  time-dependent hydrodynamical atmosphere models of a solar-type star:
  without scattering, with continuum scattering only, and with both
  continuum and line scattering. <BR /> Results: We show that continuum
  scattering does not have a significant impact on the photospheric
  temperature structure for a star like the Sun. Including scattering in
  line-blanketing, however, leads to a decrease of temperatures by about
  350 K below log<SUB>10</SUB> τ<SUB>5000</SUB> ⪉ -4. The effect is
  opposite to that of 1D hydrostatic models in radiative equilibrium,
  where scattering reduces the cooling effect of strong LTE lines in
  the higher layers of the photosphere. Coherent line scattering also
  changes the temperature distribution in the high atmosphere, where
  we observe stronger fluctuations compared to a treatment of lines as
  true absorbers.

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Title: Photon scattering 3D radiation-hydrodynamical simulations of
    late-type stellar atmospheres
Authors: Hayek, Wolfgang Simon
2010PhDT.......323H    Altcode:
  No abstract at ADS

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Title: Photon Scattering in 3D Radiative MHD Simulations
Authors: Hayek, Wolfgang
2009AIPC.1171..309H    Altcode:
  Recent results from 3D time-dependent radiative hydrodynamic
  simulations of stellar atmospheres are presented, which include
  the effects of coherent scattering in the radiative transfer
  treatment. Rayleigh scattering and electron scattering are accounted
  for in the source function, requiring an iterative solution of the
  transfer equation. Opacities and scattering coefficients are treated
  in the multigroup opacity approximation. The impact of scattering
  on the horizontal mean temperature structure is investigated, which
  is an important diagnostic for model atmospheres, with implications
  for line formation and stellar abundance measurements. <P />We find
  that continuum scattering is not important for the atmosphere of a
  metal-poor Sun with metailicity [Fe/H] = -3.0, similar to the previously
  investigated photosphere at solar metallicity.

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Title: The Hamburg/ESO R-process enhanced star survey
    (HERES). IV. Detailed abundance analysis and age dating of the
    strongly r-process enhanced stars CS 29491-069 and HE 1219-0312
Authors: Hayek, W.; Wiesendahl, U.; Christlieb, N.; Eriksson, K.;
   Korn, A. J.; Barklem, P. S.; Hill, V.; Beers, T. C.; Farouqi, K.;
   Pfeiffer, B.; Kratz, K. -L.
2009A&A...504..511H    Altcode: 2009arXiv0910.0707H
  We report on a detailed abundance analysis of two strongly
  r-process enhanced, very metal-poor stars newly discovered in
  the HERES project, <ASTROBJ>CS 29491-069</ASTROBJ> ([Fe/H]=-2.51,
  [r/Fe]=+1.1) and <ASTROBJ>HE 1219-0312</ASTROBJ> ([Fe/H]=-2.96,
  [r/Fe]=+1.5). The analysis is based on high-quality VLT/UVES spectra
  and MARCS model atmospheres. We detect lines of 15 heavy elements in
  the spectrum of <ASTROBJ>CS 29491-069</ASTROBJ>, and 18 in <ASTROBJ>HE
  1219-0312</ASTROBJ>; in both cases including the Th II 4019 Å
  line. The heavy-element abundance patterns of these two stars are
  mostly well-matched to scaled solar residual abundances not formed
  by the s-process. We also compare the observed pattern with recent
  high-entropy wind (HEW) calculations, which assume core-collapse
  supernovae of massive stars as the astrophysical environment for the
  r-process, and find good agreement for most lanthanides. The abundance
  ratios of the lighter elements strontium, yttrium, and zirconium, which
  are presumably not formed by the main r-process, are reproduced well by
  the model. Radioactive dating for <ASTROBJ>CS 29491-069</ASTROBJ> with
  the observed thorium and rare-earth element abundance pairs results in
  an average age of 9.5 Gyr, when based on solar r-process residuals, and
  17.6 Gyr, when using HEW model predictions. Chronometry seems to fail
  in the case of <ASTROBJ>HE 1219-0312</ASTROBJ>, resulting in a negative
  age due to its high thorium abundance. <ASTROBJ>HE 1219-0312</ASTROBJ>
  could therefore exhibit an overabundance of the heaviest elements,
  which is sometimes called an “actinide boost”. <P />Based on
  observations collected at the European Southern Observatory, Paranal,
  Chile (Proposal Number 170.D-0010). Table 8 is only available in
  electronic form at http://www.aanda.org

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Title: Abundance analysis of the halo giant HD 122563 with
    three-dimensional model stellar atmospheres
Authors: Collet, R.; Nordlund, Å.; Asplund, M.; Hayek, W.;
   Trampedach, R.
2009MmSAI..80..719C    Altcode: 2009arXiv0909.0690C
  We present a preliminary local thermodynamic equilibrium (LTE) abundance
  analysis of the template halo red giant HD122563 based on a realistic,
  three-dimensional (3D), time-dependent, hydrodynamical model atmosphere
  of the very metal-poor star. We compare the results of the 3D analysis
  with the abundances derived by means of a standard LTE analysis based
  on a classical, 1D, hydrostatic model atmosphere of the star. Due to
  the different upper photospheric temperature stratifications predicted
  by 1D and 3D models, we find large, negative, 3D-1D LTE abundance
  differences for low-excitation OH and Fe I lines. We also find trends
  with lower excitation potential in the derived Fe LTE abundances
  from Fe I lines, in both the 1D and 3D analyses. Such trends may be
  attributed to the neglected departures from LTE in the spectral line
  formation calculations.

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Title: First 3D radiative transfer with scattering for
    domain-decomposed MHD simulations
Authors: Hayek, W.
2008PhST..133a4006H    Altcode:
  This paper presents an implementation of the Gauss Seidel solver
  for radiative transfer with scattering in the Oslo Stagger Code. It
  fully supports MPI parallelism through domain decomposition of the
  simulation box, enabling fast computation of radiative transfer at a
  high resolution. Continuum and line opacities are treated with either a
  multigroup method or opacity sampling. Line scattering probabilities are
  estimated using the van Regemorter approximation for de-excitation rates
  of electron collisions. A solar-type test simulation with continuum
  and line scattering exhibits a steeper temperature gradient due to
  decreased radiative heating above the optical surface when compared with
  the strict local thermodynamic equilibrium (LTE) case. The classical
  van Regemorter approximation may overestimate the importance of line
  scattering, implying that the true temperature structure will be in
  between the LTE case and the scattering case considered here. It is
  demonstrated that continuum scattering is unimportant in the case of
  the Sun.