explanation      blue bibcodes open ADS page with paths to full text
Author name code: steffen
ADS astronomy entries on 2022-09-14
author:"Steffen, Matthias" 

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Title: Barium lines in high-quality spectra of two metal-poor giants
    in the Galactic halo
Authors: Cescutti, G.; Morossi, C.; Franchini, M.; Di Marcantonio, P.;
   Chiappini, C.; Steffen, M.; Valentini, M.; François, P.; Christlieb,
   N.; Cortés, C.; Kobayashi, C.; Depagne, E.
2021A&A...654A.164C    Altcode: 2021arXiv210900277C
  Context. Theoretical results showed the possibility that neutron capture
  elements were produced in the early Universe by two different sources:
  a frequent s-process source hosted by rotating massive stars, and a
  rare r-process source hosted most likely by neutron star mergers. The
  two sources produce barium with different isotopic compositions. <BR
  /> Aims: We aim to investigate the lines of barium in two halo stars,
  HD 6268 and HD 4306. The spectra present an exquisite quality, both in
  terms of resolution (R &gt; 100 000) and signal-to-noise (~400). Due
  to hyperfine splitting (hfs) effects, barium lines are expected to
  show slightly different profiles depending on the barium isotopic
  fraction. <BR /> Methods: We applied a standard local thermodynamic
  equilibrium synthesis of the barium lines. We compared the synthetic
  results assuming an s-process isotopic pattern or an r-process isotopic
  pattern for the two barium lines for each star that exhibited hfs. We
  also applied a methodology, less dependent on the accuracy of the
  theoretical Ba hfs structure, that transforms the lines of HD 4306
  into those we would observe if its atmospheric parameter values
  (i.e. T<SUB>eff</SUB>, log g, micro- and macro-turbulence, V sin i,
  and Ba abundance) were the same as those of HD 6268. <BR /> Results:
  With both methods, our results show that the barium lines with hfs
  effects of HD 4306 are in agreement with an s-process composition
  and the lines in HD 6268 have a different profile, which is most
  likely linked to the presence of an r-process isotopic pattern. <BR
  /> Conclusions: Two lines of barium of HD 6268 and HD 4306 seem to
  confirm the theoretical expectation that both r-process events and
  also s-process contribution by rotating massive stars have polluted
  the ancient halo of our Galaxy. <P />Based on observations made with
  the UVES at the ESO Very Large Telescope, Paranal Observatory, Chile
  (ID 098.B-0094(A); P.I. G. Cescutti).

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Title: The metal-poor end of the Spite plateau. II. Chemical and
    dynamical investigation
Authors: Matas Pinto, A. M.; Spite, M.; Caffau, E.; Bonifacio, P.;
   Sbordone, L.; Sivarani, T.; Steffen, M.; Spite, F.; François, P.;
   Di Matteo, P.
2021A&A...654A.170M    Altcode: 2021arXiv211000243M
  Context. The study of old, metal-poor stars deepens our knowledge on
  the early stages of the universe. In particular, the study of these
  stars gives us a valuable insight into the masses of the first massive
  stars and their emission of ionising photons. <BR /> Aims: We present
  a detailed chemical analysis and determination of the kinematic and
  orbital properties of a sample of 11 dwarf stars. These are metal-poor
  stars, and a few of them present a low lithium content. We inspected
  whether the other elements also present anomalies. <BR /> Methods:
  We analysed the high-resolution UVES spectra of a few metal-poor stars
  using the Turbospectrum code to synthesise spectral lines profiles. This
  allowed us to derive a detailed chemical analysis of Fe, C, Li, Na,
  Mg, Al, Si, CaI, CaII, ScII, TiII, Cr, Mn, Co, Ni, Sr, and Ba. <BR />
  Results: We find excellent coherence with the reference metal-poor First
  Stars sample. The lithium-poor stars do not present any anomaly of the
  abundance of the elements other than lithium. Among the Li-poor stars,
  we show that CS 22882-027 is very probably a blue-straggler. The star
  CS 30302-145, which has a Li abundance compatible with the plateau,
  has a very low Si abundance and a high Mn abundance. In many aspects,
  it is similar to the α-poor star HE 1424-0241, but it is less
  extreme. It could have been formed in a satellite galaxy and later
  been accreted by our Galaxy. This hypothesis is also supported by
  its kinematics. <P />The table with equivalent widths discussed in
  this paper is only available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr/">cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/654/A170">http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/654/A170</A>
  <P />Based on observations collected at the European Organisation for
  Astronomical Research in the Southern Hemisphere (Programmes 076.A-0463
  PI(Lopez), 077.D-0299 PI(Bonifacio)), 086.D-0871(A) (PI Meléndez).

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Title: VizieR Online Data Catalog: Abundances of metal-poor stars
    (Matas Pinto+, 2021)
Authors: Matas Pinto, A. M.; Spite, M.; Caffau, E.; Bonifacio, P.;
   Sbordone, L.; Sivarani, T.; Steffen, M.; Spite, F.; Francois, P.;
   Di Matteo, P.
2021yCat..36540170M    Altcode:
  The observations of the stars we studied are described in detail in
  Paper I (Sbordone et al., 2010A&amp;A...522A..26S, Cat. J/A+A/522/A26)
  (see their Table 1). <P />Briefly, observations were performed with
  the high-resolution spectrograph UVES at the ESO-VLT. The spectra have
  a resolving power R=~40000 and were centred at 390nm (spectral range:
  330-451nm) and 580nm (spectral range: 479-680nm). For two stars (BS
  17572-100 and HE 1413-1954) that were previously studied in the frame
  of the HERES program (Christlieb et al., 2004A&amp;A...428.1027C;
  Barklem et al., 2005A&amp;A...439..129B, Cat. J/A+A/439/129) from
  UVES spectra centred at 437nm (spectral range: 376-497nm), the blue
  spectra were centred at 346 nm (spectral range: 320-386nm). The S/N of
  the spectra at 400nm is only about half of the S/N measured at 670nm
  (see Table 1 in Paper I) and thus generally does not exceed 50. For
  two stars, CS 22188-033 and HE 0148-2611, new UVES spectra from the
  ESO archives, centred at 390 and 580nm, were also used, increasing
  the S/N ratio of the mean spectrum. The data were reduced using the
  standard UVES pipeline with the same procedures as used in Bonifacio
  et al. (2007A&amp;A...462..851B). <P />Here we present the table with
  equivalent widths discussed in the paper. <P />(2 data files).

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Title: The Gaia RVS benchmark stars. I. Chemical inventory of the
    first sample of evolved stars and its Rb NLTE investigation
Authors: Caffau, E.; Bonifacio, P.; Korotin, S. A.; François,
   P.; Lallement, R.; Matas Pinto, A. M.; Di Matteo, P.; Steffen, M.;
   Mucciarelli, A.; Katz, D.; Haywood, M.; Chemin, L.; Sartoretti, P.;
   Sbordone, L.; Andrievsky, S. M.; Kovtyukh, V. V.; Spite, M.; Spite,
   F.; Panuzzo, P.; Royer, F.; Thévenin, F.; Ludwig, H. -G.; Marchal,
   O.; Plum, G.
2021A&A...651A..20C    Altcode:
  Context. The Radial Velocity Spectrometer (RVS) on board the Gaia
  satellite is not provided with a wavelength calibration lamp. It uses
  its observations of stars with known radial velocity to derive the
  dispersion relation. To derive an accurate radial velocity calibration,
  a precise knowledge of the line spread function (LSF) of the RVS is
  necessary. Good-quality ground-based observations in the wavelength
  range of the RVS are highly desired to determine the LSF. <BR /> Aims:
  Several radial velocity standard stars are available to the Gaia
  community. The highest possible number of calibrators will surely
  allow us to improve the accuracy of the radial velocity. Because
  the LSF may vary across the focal plane of the RVS, a large number
  of high-quality spectra for the LSF calibration may allow us to
  better sample the properties of the focal plane. <BR /> Methods:
  We selected a sample of stars to be observed with UVES at the Very
  Large Telescope, in a setting including the wavelength range of RVS,
  that are bright enough to allow obtaining high-quality spectra in a
  short time. We also selected stars that lack chemical investigation in
  order to increase the sample of bright, close by stars with a complete
  chemical inventory. <BR /> Results: We here present the chemical
  analysis of the first sample of 80 evolved stars. The quality of the
  spectra is very good, therefore we were able to derive abundances for
  20 elements. The metallicity range spanned by the sample is about 1
  dex, from slightly metal-poor to solar metallicity. We derived the
  Rb abundance for all stars and investigated departures from local
  thermodynamical equilibrium (NLTE) in the formation of its lines. <BR />
  Conclusions: The sample of spectra is of good quality, which is useful
  for a Gaia radial velocity calibration. The Rb NLTE effects in this
  stellar parameters range are small but sometimes non-negligible,
  especially for spectra of this good quality. <P />Tables B.3
  and C.1 are only available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr">cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/651/A20">http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/651/A20</A>
  <P />Based on observations made with UVES at VLT 104.D.0325.

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Title: VizieR Online Data Catalog: Gaia RVS benchmark
    stars. I. (Caffau+, 2021)
Authors: Caffau, E.; Bonifacio, P.; Korotin, S. A.; Francois, P.;
   Lallement, R.; Matas Pinto, A. M.; Di Matteo, P.; Steffen, M.;
   Mucciarelli, A.; Katz, D.; Haywood, M.; Chemin, L.; Sartoretti, P.;
   Sbordone, L.; Andrievsky, S. M.; Kovtyukh, V. V.; Spite, M.; Spite,
   F.; Panuzzo, P.; Royer, F.; Thevenin, F.; Ludwig, H. -G.; Marchal,
   O.; Plum, G.
2021yCat..36510020C    Altcode:
  For this project on the UVES spectrograph, we selected the setting
  437+760. The choices on the setting were that (i) the 760 range
  completely covers the RVS range without any gaps, and (ii) the 437 range
  is the reddest setting that can be coupled with the 760 setting. For
  metal-rich stars (the majority of our targets), observations in
  blue settings provide very crowded spectra, and a higher S/N can be
  achieved in this selected setting than in bluer settings such as the
  390 setting. <P />We chose the highest UVES resolution (slit 0.4"
  in the blue arm and 0.3" in the red arm). For all observations, the
  DIC2 437+760 setting was used. For the stars brighter than V magnitude
  8.5, an observing block comprises ten observations of 77.5s to avoid
  detector saturation. For the stars fainter than 8.5, five exposures of
  202 s allow avoiding detector saturation. In this program, 90 stars
  have been observed, 80 of which are evolved stars and are analysed
  here. The 10 unevolved stars will be analysed with stars of similar
  stellar parameters that are observed or are scheduled to be observed
  for the following two ESO periods (P105 and P106). <P />(2 data files).

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Title: 3D spectroscopic analysis of helium-line white dwarfs
Authors: Cukanovaite, Elena; Tremblay, Pier-Emmanuel; Bergeron,
   Pierre; Freytag, Bernd; Ludwig, Hans-Günter; Steffen, Matthias
2021MNRAS.501.5274C    Altcode: 2020arXiv201112693C; 2020MNRAS.tmp.3465C
  In this paper, we present corrections to the spectroscopic parameters
  of DB and DBA white dwarfs with -10.0 ≤ log (H/He) ≤ -2.0, 7.5
  ≤ log g ≤ 9.0, and $12\, 000$ ≲ T<SUB>eff</SUB> $\lesssim 34\,
  000\,\mathrm{ K}$ , based on 282 3D atmospheric models calculated with
  the CO<SUP>5</SUP>BOLD radiation-hydrodynamics code. These corrections
  arise due to a better physical treatment of convective energy transport
  in 3D models when compared to the previously available 1D model
  atmospheres. By applying the corrections to an existing Sloan Digital
  Sky Survey (SDSS) sample of DB and DBA white dwarfs, we find significant
  corrections both for effective temperature and surface gravity. The
  3D log g corrections are most significant for T<SUB>eff</SUB> ≲
  18 000 K, reaching up to -0.20 dex at log g = 8.0. However, in this
  low effective temperature range, the surface gravity determined from
  the spectroscopic technique can also be significantly affected by
  the treatment of the neutral van der Waals line broadening of helium
  and by non-ideal effects due to the perturbation of helium by neutral
  atoms. Thus, by removing uncertainties due to 1D convection, our work
  showcases the need for improved description of microphysics for DB
  and DBA model atmospheres. Overall, we find that our 3D spectroscopic
  parameters for the SDSS sample are generally in agreement with Gaia
  Data Release 2 absolute fluxes within 1σ-3σ for individual white
  dwarfs. By comparing our results to DA white dwarfs, we determine
  that the precision and accuracy of DB/DBA atmospheric models are
  similar. For ease of user application of the correction functions,
  we provide an example PYTHON code.

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Title: The solar gravitational redshift from HARPS-LFC Moon
    spectra⋆. A test of the general theory of relativity
Authors: González Hernández, J. I.; Rebolo, R.; Pasquini, L.;
   Lo Curto, G.; Molaro, P.; Caffau, E.; Ludwig, H. -G.; Steffen, M.;
   Esposito, M.; Suárez Mascareño, A.; Toledo-Padrón, B.; Probst,
   R. A.; Hänsch, T. W.; Holzwarth, R.; Manescau, A.; Steinmetz, T.;
   Udem, Th.; Wilken, T.
2020A&A...643A.146G    Altcode: 2020arXiv200910558G
  Context. The general theory of relativity predicts the redshift of
  spectral lines in the solar photosphere as a consequence of the
  gravitational potential of the Sun. This effect can be measured
  from a solar disk-integrated flux spectrum of the Sun's reflected
  light on Solar System bodies. <BR /> Aims: The laser frequency comb
  (LFC) calibration system attached to the HARPS spectrograph offers
  the possibility of performing an accurate measurement of the solar
  gravitational redshift (GRS) by observing the Moon or other Solar System
  bodies. Here, we analyse the line shift observed in Fe absorption lines
  from five high-quality HARPS-LFC spectra of the Moon. <BR /> Methods:
  We selected an initial sample of 326 photospheric Fe lines in the
  spectral range between 476-585 nm and measured their line positions
  and equivalent widths (EWs). Accurate line shifts were derived from
  the wavelength position of the core of the lines compared with the
  laboratory wavelengths of Fe lines. We also used a CO<SUP>5</SUP>BOLD
  3D hydrodynamical model atmosphere of the Sun to compute 3D synthetic
  line profiles of a subsample of about 200 spectral Fe lines centred
  at their laboratory wavelengths. We fit the observed relatively
  weak spectral Fe lines (with EW&lt; 180 mÅ) with the 3D synthetic
  profiles. <BR /> Results: Convective motions in the solar photosphere
  do not affect the line cores of Fe lines stronger than about ∼150
  mÅ. In our sample, only 15 Fe I lines have EWs in the range 150&lt;
  EW(mÅ) &lt; 550, providing a measurement of the solar GRS at 639 ±
  14 m s<SUP>-1</SUP>, which is consistent with the expected theoretical
  value on Earth of ∼633.1 m s<SUP>-1</SUP>. A final sample of about 97
  weak Fe lines with EW &lt; 180 mÅ allows us to derive a mean global
  line shift of 638 ± 6 m s<SUP>-1</SUP>, which is in agreement with
  the theoretical solar GRS. <BR /> Conclusions: These are the most
  accurate measurements of the solar GRS obtained thus far. Ultrastable
  spectrographs calibrated with the LFC over a larger spectral range,
  such as HARPS or ESPRESSO, together with a further improvement on the
  laboratory wavelengths, could provide a more robust measurement of the
  solar GRS and further testing of 3D hydrodynamical models. <P />Tables
  A.1 and A.2 are only available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr/">http://cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/643/A146">http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/643/A146</A>
  <P />Based on observations taken with the ESO 3.6 m telescope at La
  Silla Observatory, Chile.

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Title: Probing the atmosphere of HD189733b with the Na I and K I lines
Authors: Keles, E.; Kitzmann, D.; Mallonn, M.; Alexoudi, X.; Fossati,
   L.; Pino, L.; Seidel, J. V.; Carroll, T. A.; Steffen, M.; Ilyin, I.;
   Poppenhäger, K.; Strassmeier, K. G.; von Essen, C.; Nascimbeni, V.;
   Turner, J. D.
2020MNRAS.498.1023K    Altcode: 2020MNRAS.tmp.2443K; 2020arXiv200804044K
  High spectral resolution transmission spectroscopy is a powerful tool to
  characterize exoplanet atmospheres. Especially for hot Jupiters, this
  technique is highly relevant, due to their high-altitude absorption,
  e.g. from resonant sodium (Na I) and potassium (K I) lines. We resolve
  the atmospheric K I absorption on HD189733b with the aim to compare
  the resolved K I line and previously obtained high-resolution Na
  I-D line observations with synthetic transmission spectra. The line
  profiles suggest atmospheric processes leading to a line broadening of
  the order of ∼10 km/s for the Na I-D lines and only a few km/s for
  the K I line. The investigation hints that either the atmosphere of
  HD189733b lacks a significant amount of K I or the alkali lines probe
  different atmospheric regions with different temperature, which could
  explain the differences we see in the resolved absorption lines.

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Title: VizieR Online Data Catalog: The solar gravitational redshift
    (Gonzalez Hernandez+, 2020)
Authors: Gonzalez Hernandez, J. I.; Rebolo, R.; Pasquini, L.; Lo Curto,
   G.; Molaro, P.; Caffau, E.; Ludwig, H. -G.; Steffen, M.; Esposito,
   M.; Suarez Mascarenno, A.; Toledo-Padron, B.; Probst, R. A.; Hansch,
   T. W.; Holzwarth, R.; Manescau, A.; Steinmetz, T.; Udem, T.; Wilken, T.
2020yCat..36430146G    Altcode:
  Line data and velocity shifts of the FeI and FeII lines,
  with laboratory wavelengths, λ<SUB>lab</SUB>, from Nave et
  al. (1994ApJS...94..221N, 2013ApJS..204....1N) and excitation
  potentials, oscillator strengths from the VALD database (Piskunov et
  al. 1995A&amp;AS..112..525P). <P />In Table A.1 we provide the mean line
  core shifts, v<SUB>core</SUB>obs, measured on the spectral lines from
  the observed HARPS-LFC spectra of the MOON and computed with respect to
  the original laboratory wavelengths (Nave et al. 1994ApJS...94..221N,
  2013ApJS..204....1N). <P />We also give the recalibrated wavelengths,
  lambda_nist, computed from recalibrated wavenumber measurements and
  Ritz wavelengths, lambda_ritz, computed from recalibrated energy levels,
  with their corresponding wavelengths uncertainties, extracted from the
  NIST database (Kramida et al. 2019APS..DMPN09004K). <P />In Table A.2,
  we give the line core shifts measured on the observed spectral lines,
  v<SUB>core</SUB>obs_n, estimated using the recalibrated wavelengths,
  lambda_nist, as reference laboratory wavelengths, the 3D profiles,
  v<SUB>core,3D, and the global line shifts, v</SUB>fit<SUB>3D</SUB>n,
  from fitting the observed spectral lines using 3D profiles, and
  corrected using the recalibrated wavelengths lambda_nist as reference
  laboratory wavelengths. <P />Wavelengths are given in Angstroms,
  wavelength uncertainties in miliAngstroems, excitation potentials in
  eV, equivalent widths (EW) in miliAngstroems, and velocity shifts in
  m/s. <P />(2 data files).

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Title: 16th Potsdam Thinkshop: The rotation periods of cool stars:
    Measurements, uses, connections and prospects
Authors: Barnes, S. A.; Steffen, M.; Strassmeier, K. G.
2020AN....341..485B    Altcode:
  No abstract at ADS

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Title: Improving spectroscopic lithium abundances. Fitting functions
    for 3D non-LTE corrections in FGK stars of different metallicity
Authors: Mott, A.; Steffen, M.; Caffau, E.; Strassmeier, K. G.
2020A&A...638A..58M    Altcode: 2020arXiv200410803M
  Context. Accurate spectroscopic lithium abundances are essential in
  addressing a variety of open questions, such as the origin of a uniform
  lithium content in the atmospheres of metal-poor stars (Spite plateau)
  or the existence of a correlation between the properties of extrasolar
  planetary systems and the lithium abundance in the atmosphere of
  their host stars. <BR /> Aims: We have developed a tool that allows
  the user to improve the accuracy of standard lithium abundance
  determinations based on 1D model atmospheres and the assumption of
  local thermodynamic equilibrium (LTE) by applying corrections that
  account for hydrodynamic (3D) and non-LTE (NLTE) effects in FGK stars
  of different metallicity. <BR /> Methods: Based on a grid of CO5BOLD
  3D models and associated 1D hydrostatic atmospheres, we computed
  three libraries of synthetic spectra of the lithium λ 670.8 nm line
  for a wide range of lithium abundances, accounting for detailed line
  formation in 3D NLTE, 1D NLTE, and 1D LTE, respectively. The resulting
  curves-of-growth were then used to derive 3D NLTE and 1D NLTE lithium
  abundance corrections. <BR /> Results: For all metallicities, the
  largest corrections are found at the coolest effective temperature,
  T<SUB>eff</SUB> = 5000 K. They are mostly positive, up to + 0.2 dex,
  for the weakest lines (lithium abundance A(Li)<SUB>1DLTE</SUB> = 1.0),
  whereas they become more negative towards lower metallicities, where
  they can reach - 0.4 dex for the strongest lines (A(Li)<SUB>1DLTE</SUB>
  = 3.0) at [Fe/H] = - 2.0. We demonstrate that 3D and NLTE effects are
  small for metal-poor stars on the Spite plateau, leading to errors of at
  most ± 0.05 dex if ignored. We present analytical functions evaluating
  the 3D NLTE and 1D NLTE corrections as a function of T<SUB>eff</SUB>
  [5000…6500 K], log g [3.5…4.5], and LTE lithium abundance A(Li)
  [1.0…3.0] for a fixed grid of metallicities [Fe/H] [ - 3.0…0.0]. In
  addition, we also provide analytical fitting functions for directly
  converting a given lithium abundance into an equivalent width, or vice
  versa, a given equivalent width (EW) into a lithium abundance. For
  convenience, a Python script is made available that evaluates all
  fitting functions for given T<SUB>eff</SUB>, log g, [Fe/H], and A(Li)
  or EW. <BR /> Conclusions: By means of the fitting functions developed
  in this work, the results of complex 3D and NLTE calculations are
  made readily accessible and quickly applicable to large samples of
  stars across a wide range of metallicities. Improving the accuracy
  of spectroscopic lithium abundance determinations will contribute to
  a better understanding of the open questions related to the lithium
  content in metal-poor and solar-like stellar atmospheres.

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Title: The <SUP>6</SUP>Li/<SUP>7</SUP>Li isotopic ratio in the
    metal-poor binary CS22876-032
Authors: González Hernández, J. I.; Bonifacio, P.; Caffau, E.;
   Ludwig, H. -G.; Steffen, M.; Monaco, L.; Cayrel, R.
2019A&A...628A.111G    Altcode: 2019arXiv190705109G
  <BR /> Aims: We present high-resolution and high-quality UVES
  spectroscopic data of the metal-poor double-lined spectroscopic binary
  CS 22876-032 ([Fe/H] approximately -3.7 dex). Our goal is to derive
  the <SUP>6</SUP>Li/<SUP>7</SUP>Li isotopic ratio by analysing the
  Li I λ 670.8 nm doublet. <BR /> Methods: We co-added all 28 useful
  spectra normalised and corrected for radial velocity to the rest frame
  of the primary star. We fitted the Li profile with a grid of the 3D
  non-local thermodynamic equilibrium (NLTE) synthetic spectra to take
  into account the line profile asymmetries induced by stellar convection,
  and performed Monte Carlo simulations to evaluate the uncertainty of
  the fit of the Li line profile. <BR /> Results: We checked that the
  veiling factor does not affect the derived isotopic ratio, <SUP>6</SUP>
  Li/<SUP>7</SUP>Li, and only modifies the Li abundance, A(Li), by
  about 0.15 dex. The best fit of the Li profile of the primary star
  provides A(Li) = 2.17 ± 0.01 dex and <SUP>6</SUP> Li/<SUP>7</SUP>Li =
  8<SUB>-5</SUB><SUP>+2</SUP>% at 68% confidence level. In addition, we
  improved the Li abundance of the secondary star at A(Li) = 1.55 ± 0.04
  dex, which is about 0.6 dex lower than that of the primary star. <BR
  /> Conclusions: The analysis of the Li profile of the primary star is
  consistent with no detection of <SUP>6</SUP> Li and provides an upper
  limit to the isotopic ratio of <SUP>6</SUP> Li/<SUP>7</SUP>Li &lt;
  10% at this very low metallicity, about 0.5 dex lower in metallicity
  than previous attempts for detection of <SUP>6</SUP> Li in extremely
  metal poor stars. These results do not solve or worsen the cosmological
  <SUP>7</SUP> Li problem, nor do they support the need for non-standard
  <SUP>6</SUP>Li production in the early Universe. <P />The two averaged
  spectra are only available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr">http://cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/628/A111">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/628/A111</A>Based
  on observations made with the Very Large Telescope (VLT) at ESO Paranal
  Observatory, Chile, Programme 080.D-0333.

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Title: VizieR Online Data Catalog: Li in BPS CS22876-032 spectrum
    (Gonzalez Hernandez+, 2019)
Authors: Gonzalez Hernandez, J. I.; Bonifacio, P.; Caffau, E.; Ludwig,
   H. -G.; Steffen, M.; Monaco, L.; Cayrel, R.
2019yCat..36280111G    Altcode:
  Average co-added, rebinned spectra in the region around the LiI 670.8nm
  resonance line of the two stellar components of the metal-poor binary
  CS 22876-032 A and CS 22876-032 B. For each star, wavelength, normalised
  flux and flux error are given. <P />(2 data files).

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Title: Confronting expansion distances of planetary nebulae with
    Gaia DR2 measurements
Authors: Schönberner, D.; Steffen, M.
2019A&A...625A.137S    Altcode: 2019arXiv190410721S
  Context. Individual distances to planetary nebulae are of the utmost
  relevance for our understanding of post-asymptotic giant-branch
  evolution because they allow a precise determination of stellar and
  nebular properties. Also, objects with individual distances serve
  as calibrators for the so-called statistical distances based on
  secondary nebular properties. <BR /> Aims: With independently known
  distances, it is possible to check empirically our understanding
  of the formation and evolution of planetary nebulae as suggested by
  existing hydrodynamical simulations. <BR /> Methods: We compared the
  expansion parallaxes that have recently been determined for a number
  of planetary nebulae with the trigonometric parallaxes provided by the
  Gaia Data Release 2. <BR /> Results: Except for two out of 11 nebulae,
  we found good agreement between the expansion and the Gaia trigonometric
  parallaxes without any systematic trend with distance. Therefore, the
  Gaia measurements also prove that the correction factors necessary
  to convert proper motions of shocks into Doppler velocities cannot
  be ignored. Rather, the size of these correction factors and their
  evolution with time as predicted by 1D hydrodynamical models of
  planetary nebulae is basically validated. These correction factors
  are generally greater than unity and are different for the outer
  shell and the inner bright rim of a planetary nebula. The Gaia
  measurements also confirm earlier findings that spectroscopic methods
  often lead to an overestimation of the distance. They also show that
  even modelling of the entire system of star and nebula by means
  of sophisticated photoionisation modelling may not always provide
  reliable results. <BR /> Conclusions: The Gaia measurements confirm
  the basic correctness of the present radiation-hydrodynamics models,
  which predict that both the shell and the rim of a planetary nebula are
  two independently expanding entities, created and driven by different
  physical processes, namely thermal pressure (shell) or wind interaction
  (rim), both of which vary differently with time. <P />This work has
  made use of data from the European Space Agency (ESA) mission Gaia (<A
  href="https://www.cosmos.esa.int/gaia">https://www.cosmos.esa.int/gaia</A>),
  processed by the Gaia Data Processing and Analysis Consortium (DPAC, <A
  href="https://www.cosmos.esa.int/web/gaia/dpac/consortium">https://www.cosmos.esa.int/web/gaia/dpac/consortium</A>).
  Funding for the DPAC has been provided by national institutions, in
  particular the institutions participating in the Gaia Multilateral
  Agreement.

---------------------------------------------------------
Title: TOPoS. V. Abundance ratios in a sample of very metal-poor
    turn-off stars
Authors: François, P.; Caffau, E.; Bonifacio, P.; Spite, M.; Spite,
   F.; Cayrel, R.; Christlieb, N.; Gallagher, A. J.; Klessen, R.; Koch,
   A.; Ludwig, H. -G.; Monaco, L.; Plez, B.; Steffen, M.; Zaggia, S.
2018A&A...620A.187F    Altcode: 2018arXiv181100035F
  Context. Extremely metal-poor stars are keys to understand the early
  evolution of our Galaxy. The ESO large programme TOPoS has been tailored
  to analyse a new set of metal-poor turn-off stars, whereas most of
  the previously known extremely metal-poor stars are giant stars. <BR
  /> Aims: Sixty five turn-off stars (preselected from SDSS spectra)
  have been observed with the X-shooter spectrograph at the ESO VLT Unit
  Telescope 2, to derive accurate and detailed abundances of magnesium,
  silicon, calcium, iron, strontium and barium. <BR /> Methods: We
  analysed medium-resolution spectra (R ≃ 10 000) obtained with the
  ESO X-shooter spectrograph and computed the abundances of several
  α and neutron-capture elements using standard one-dimensional local
  thermodynamic equilibrium (1D LTE) model atmospheres. <BR /> Results:
  Our results confirms the super-solar [Mg/Fe] and [Ca/Fe] ratios in
  metal-poor turn-off stars as observed in metal-poor giant stars. We
  found a significant spread of the [α/Fe] ratios with several stars
  showing subsolar [Ca/Fe] ratios. We could measure the abundance of
  strontium in 12 stars of the sample, leading to abundance ratios
  [Sr/Fe] around the Solar value. We detected barium in two stars
  of the sample. One of the stars (SDSS J114424-004658) shows both
  very high [Ba/Fe] and [Sr/Fe] abundance ratios (&gt;1 dex). <P
  />Based on observations collected at the European Organisation for
  Astronomical Research in the Southern Hemisphere under ESO programme ID
  189.D-0165. <P />Equivalent widths of the Fe lines are only, and Tables
  A.1 and A.2 are also 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/620/A187">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/620/A187</A>

---------------------------------------------------------
Title: Hot bubbles of planetary nebulae with hydrogen-deficient
    winds. II. Analytical approximations with application to BD + 30°3639
Authors: Heller, R.; Jacob, R.; Schönberner, D.; Steffen, M.
2018A&A...620A..98H    Altcode: 2018arXiv180908305H
  Context. The first high-resolution X-ray spectroscopy of a planetary
  nebula, BD +30° 3639, opened the possibility to study plasma conditions
  and chemical compositions of X-ray emitting "hot" bubbles of planetary
  nebulae in much greater detail than before. <BR /> Aims: We investigate
  (i) how diagnostic line ratios are influenced by the bubble's thermal
  structure and chemical profile, (ii) whether the chemical composition
  inside the bubble of BD +30° 3639 is consistent with the hydrogen-poor
  composition of the stellar photosphere and wind, and (iii) whether
  hydrogen-rich nebular matter has already been added to the bubble of BD
  +30° 3639 by evaporation. <BR /> Methods: We applied an analytical,
  one-dimensional (1D) model for wind-blown bubbles with temperature
  and density profiles based on self-similar solutions including
  thermal conduction. We also constructed heat-conduction bubbles with
  a chemical stratification. The X-ray emission was computed using the
  well-documented CHIANTI code. These bubble models are used to re-analyse
  the high-resolution X-ray spectrum from the hot bubble of BD +30°
  3639. <BR /> Results: We found that our 1D heat-conducting bubble
  models reproduce the observed line ratios much better than plasmas
  with single electron temperatures. In particular, all the temperature-
  and abundance-sensitive line ratios are consistent with BD +30° 3639
  X-ray observations for (i) an intervening column density of neutral
  hydrogen, N<SUB>H</SUB> = 0.20<SUB>-0.10</SUB><SUP>+0.05</SUP> ×
  10<SUP>22</SUP>cm<SUP>-2</SUP>, (ii) a characteristic bubble X-ray
  temperature of T<SUB>X</SUB> = 1.8 ± 0.1 MK together with (iii)
  a very high neon mass fraction of about 0.05, virtually as high as
  that of oxygen. For lower values of N<SUB>H</SUB>, we cannot exclude
  the possibility that the hot bubble of BD +30° 3639 contains a small
  amount of "evaporated" (or mixed) hydrogen-rich nebular matter. Given
  the possible range of N<SUB>H</SUB>, the fraction of evaporated
  hydrogen-rich matter cannot exceed 3% of the bubble mass. <BR />
  Conclusions: The diffuse X-ray emission from BD +30° 3639 can be well
  explained by models of wind-blown bubbles with thermal conduction and
  a chemical composition equal to that of the hydrogen-poor and carbon-,
  oxygen-, and neon-rich stellar surface.

---------------------------------------------------------
Title: VizieR Online Data Catalog: Very metal-poor turn-off stars
    abundances (Francois+, 2018)
Authors: Francois, P.; Caffau, E.; Bonifacio, P.; Spite, M.; Spite,
   F.; Cayrel, R.; Christlieb, N.; Gallagher, A.; Klessen, R.; Koch,
   A.; Ludwig, H. -G.; Monaco, L.; Plez, B.; Steffen, M.; Zaggia, S.
2018yCat..36200187F    Altcode:
  Sixty five turn-off stars (preselected from SDSS spectra) have been
  observed with the X-Shooter spectrograph at the ESO VLT Unit Telescope
  2, to derive accurate and detailed abundances of magnesium, silicon,
  calcium, iron, strontium and barium. We analysed medium-resolution
  spectra (R~10000) obtained with the ESO X-Shooter spectrograph and
  computed the abundances of several alpha and neutron-capture elements
  using standard one-dimensional local thermodynamic equilibrium (1D LTE)
  model atmospheres. <P />(3 data files).

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Title: 3D non-LTE corrections for Li abundance and
    <SUP>6</SUP>Li/<SUP>7</SUP>Li isotopic ratio in solar-type
    stars. I. Application to HD 207129 and HD 95456
Authors: Harutyunyan, G.; Steffen, M.; Mott, A.; Caffau, E.; Israelian,
   G.; González Hernández, J. I.; Strassmeier, K. G.
2018A&A...618A..16H    Altcode: 2018arXiv180704089H
  Context. Convective motions in solar-type stellar atmospheres
  induce Doppler shifts that affect the strengths and shapes of
  spectral absorption lines and create slightly asymmetric line
  profiles. One-dimensional (1D) local thermodynamic equilibrium
  (LTE) studies of elemental abundances are not able to reproduce this
  phenomenon, which becomes particularly important when modeling the
  impact of isotopic fine structure, like the subtle depression created by
  the <SUP>6</SUP>Li isotope on the red wing of the Li I resonance doublet
  line. <BR /> Aims: The purpose of this work is to provide corrections
  for the lithium abundance, A(Li), and the <SUP>6</SUP>Li/<SUP>7</SUP>Li
  isotopic ratio that can easily be applied to correct 1D LTE lithium
  abundances in G and F dwarf stars of approximately solar mass and
  metallicity for three-dimensional (3D) and non-LTE (NLTE) effects. <BR
  /> Methods: The corrections for A(Li) and <SUP>6</SUP>Li/<SUP>7</SUP>Li
  are computed using grids of 3D NLTE and 1D LTE synthetic lithium
  line profiles, generated from 3D hydro-dynamical CO<SUP>5</SUP>BOLD
  and 1D hydrostatic model atmospheres, respectively. For comparative
  purposes, all calculations are performed for three different line
  lists representing the Li I λ670.8 nm spectral region. The 3D NLTE
  corrections are then approximated by analytical expressions as a
  function of the stellar parameters (T<SUB>eff</SUB>, log ℊ, [Fe/H],
  ν sin i, A(Li), <SUP>6</SUP>Li/<SUP>7</SUP>Li). These are applied to
  adjust the 1D LTE isotopic lithium abundances in two solar-type stars,
  <ASTROBJ>HD 207129</ASTROBJ> and <ASTROBJ>HD 95456</ASTROBJ>, for
  which high-quality HARPS observations are available. <BR /> Results:
  The derived 3D NLTE corrections range between -0.01 and +0.11 dex for
  A(Li), and between -4.9 and -0.4% for <SUP>6</SUP>Li/<SUP>7</SUP>Li,
  depending on the adopted stellar parameters. We confirm that the
  inferred <SUP>6</SUP>Li abundance depends critically on the strength of
  the Si I 670.8025 nm line. Our findings show a general consistency with
  recent works on lithium abundance corrections. After the application of
  such corrections, we do not find a significant amount of <SUP>6</SUP>Li
  in any of the two target stars. <BR /> Conclusions: In the case of
  <SUP>6</SUP>Li/<SUP>7</SUP>Li, our corrections are always negative,
  showing that 1D LTE analysis can significantly overestimate the
  presence of <SUP>6</SUP>Li (up to 4.9% points) in the atmospheres
  of solar-like dwarf stars. These results emphasize the importance
  of reliable 3D model atmospheres combined with NLTE line formation
  for deriving precise isotopic lithium abundances. Although 3D NLTE
  spectral synthesis implies an extensive computational effort,
  the results can be made accessible with parametric tools like
  the ones presented in this work. <P />The table with the 3D NLTE
  corrections is only available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr">http://cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/618/A16">http://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/618/A16</A>

---------------------------------------------------------
Title: Abundance of zinc in the red giants of Galactic globular
    cluster 47 Tucanae
Authors: Černiauskas, A.; Kučinskas, A.; Klevas, J.; Bonifacio,
   P.; Ludwig, H. -G.; Caffau, E.; Steffen, M.
2018A&A...616A.142C    Altcode: 2018arXiv180603132C
  <BR /> Aims: We investigate possible relations between the abundances
  of zinc and the light elements sodium, magnesium, and potassium
  in the atmospheres of red giant branch (RGB) stars of the Galactic
  globular cluster 47 Tuc and study connections between the chemical
  composition and dynamical properties of the cluster RGB stars. <BR
  /> Methods: The abundance of zinc was determined in 27 RGB stars
  of 47 Tuc using 1D local thermal equilibrium (LTE) synthetic line
  profile fitting to the high-resolution 2dF/HERMES spectra obtained
  with the Anglo-Australian Telescope (AAT). Synthetic spectra used
  in the fitting procedure were computed with the SYNTHE code and
  1D ATLAS9 stellar model atmospheres. <BR /> Results: The average
  1D LTE zinc-to-iron abundance ratio and its RMS variations due to
  star-to-star abundance spread determined in the sample of 27 RGB stars
  is &lt;[Zn/Fe]&gt;<SUP>1D LTE</SUP> = 0.11 ± 0.09. We did not detect
  any statistically significant relations between the abundances of
  zinc and those of light elements. Neither did we find any significant
  correlation or anticorrelation between the zinc abundance in individual
  stars and their projected distance from the cluster center. Finally,
  no statistically significant relation between the absolute radial
  velocities of individual stars and the abundance of zinc in their
  atmospheres was detected. The obtained average [Zn/Fe]<SUP>1DLTE</SUP>
  ratio agrees well with those determined in this cluster in earlier
  studies and nearly coincides with that of Galactic field stars at this
  metallicity. All these results suggest that nucleosynthesis of zinc
  and light elements proceeded in separate, unrelated pathways in 47 Tuc.

---------------------------------------------------------
Title: Carbon-enhanced metal-poor 3D model atmospheres
Authors: Steffen, M.; Gallagher, A. J.; Caffau, E.; Bonifacio, P.;
   Ludwig, H. -G.
2018IAUS..334..364S    Altcode: 2017arXiv170805686S
  We present our latest 3D model atmospheres for carbon-enhanced
  metal-poor (CEMP) stars computed with the CO5BOLD code. The stellar
  parameters are representative of hot turn-off objects (T<SUB>eff</SUB>
  ~ 6250 K, log g = 4.0, [Fe/H]=-3). The main purpose of these models
  is to investigate the role of 3D effects on synthetic spectra of the
  CH G-band (4140-4400 Å), the CN BX-band (3870-3890 Å), and several
  UV OH transitions (3122-3128 Å). By comparison with the synthetic
  spectra from standard 1D model atmospheres (assuming local thermodynamic
  equilibrium, LTE), we derive 3D abundance corrections for carbon and
  oxygen of up to -0.5 and -0.7 dex, respectively.

---------------------------------------------------------
Title: Abundances of Mg and K in the atmospheres of turn-off starsin
    Galactic globular cluster 47 Tucanae
Authors: Černiauskas, A.; Kučinskas, A.; Klevas, J.; Dobrovolskas,
   V.; Korotin, S.; Bonifacio, P.; Ludwig, H. -G.; Caffau, E.; Steffen, M.
2018A&A...615A.173C    Altcode: 2018arXiv180410033C
  <BR /> Aims: We determined abundances of Mg and K in the atmospheres
  of 53 (Mg) and 75 (K) turn-off (TO) stars of the Galactic globular
  cluster 47 Tuc. The obtained abundances, together with those of Li,
  O, and Na that we had earlier determined for the same sample of stars,
  were used to search for possible relations between the abundances of K
  and other light elements, Li, O, Na, and Mg, as well as the connections
  between the chemical composition of TO stars and their kinematical
  properties. <BR /> Methods: Abundances of Mg and K were determined using
  archival high resolution VLT FLAMES/GIRAFFE spectra, in combination
  with the one-dimensional (1D) non-local thermodynamic equilibrium
  (NLTE) spectral synthesis methodology. Spectral line profiles were
  computed with the MULTI code, using 1D hydrostatic ATLAS9 stellar model
  atmospheres. We also utilized three-dimensional (3D) hydrodynamical
  CO<SUP>5</SUP>BOLD and 1D hydrostatic LHD model atmospheres for
  computing 3D-1D LTE abundance corrections for the spectral lines
  of Mg and K, in order to assess the influence of convection on their
  formation in the atmospheres of TO stars. <BR /> Results: The determined
  average abundance-to-iron ratios and their root mean square variations
  due to star-to-star abundance spreads were &lt;[Mg/Fe]&gt;<SUP>1D
  NLTE</SUP> = 0.47 ± 0.12, and &lt;[K/Fe]&gt;<SUP>1D NLTE</SUP> = 0.39
  ± 0.09. Although the data suggest the possible existence of a weak
  correlation in the [K/Fe]-[Na/Fe] plane, its statistical significance
  is low. No statistically significant relations between the abundance
  of K and other light elements were detected. Also, we did not find any
  significant correlations or anti-correlations between the [Mg/Fe] and
  [K/Fe] ratios and projected distance from the cluster center. Similarly,
  no relations between the absolute radial velocities of individual stars
  and abundances of Mg and K in their atmospheres were detected. The
  3D-1D abundance corrections were found to be small (≤0.1 dex) for
  the lines of Mg and K used in this study, thus indicating that the
  influence of convection on their formation is small.

---------------------------------------------------------
Title: VizieR Online Data Catalog: A(Li) and 6Li/7Li 3D NLTE
    corrections (Harutyunyan+, 2018)
Authors: Harutyunyan, G.; Steffen, M.; Mott, A.; Caffau, E.; Israelian,
   G.; Gonzalez Hernandez, J. I.; Strassmeier, K. G.
2018yCat..36180016H    Altcode:
  A grid of 3D non-LTE (NLTE) corrections for the lithium abundance,
  A(Li), and the <SUP>6</SUP>Li/<SUP>7</SUP>Li isotopic ratio are
  presented. These corrections can be easily applied to correct 1D
  LTE lithium abundances in G and F dwarf stars of approximately
  solar mass and metallicity for 3D and NLTE effects. The stellar
  parameters defining the grid are effective temperatures, Teff (5900,
  6300 and 6500K), surface gravity, logg (4.0 and 4.5), metallicity,
  [Fe/H] (-1.0, -0.5, 0.0, +0.5), 1D LTE lithium abundance, A(Li)
  (1.5, 2.0, 2.5), 1D LTE <SUP>6</SUP>Li/<SUP>7</SUP>Li isotopic ratio
  (0, 5 and 10%), as well as projected rotational velocity, vsini (0,
  2, 4 and 6km/s). Based on this table, a web page calculator was
  created that allows to compute the 3D NLTE corrections of A(Li)
  and 6Li/7Li ratio for a given combination of stellar parameters
  (https://pages.aip.de/li67nlte3d/). <P />(1 data file).

---------------------------------------------------------
Title: Simulation of the small-scale magnetism in main-sequence
    stellar atmospheres
Authors: Salhab, R. G.; Steiner, O.; Berdyugina, S. V.; Freytag, B.;
   Rajaguru, S. P.; Steffen, M.
2018A&A...614A..78S    Altcode:
  Context. Observations of the Sun tell us that its granular and
  subgranular small-scale magnetism has significant consequences for
  global quantities such as the total solar irradiance or convective
  blueshift of spectral lines. <BR /> Aims: In this paper, properties
  of the small-scale magnetism of four cool stellar atmospheres,
  including the Sun, are investigated, and in particular its effects
  on the radiative intensity and flux. <BR /> Methods: We carried out
  three-dimensional radiation magnetohydrodynamic simulations with the
  CO<SUP>5</SUP>BOLD code in two different settings: with and without
  a magnetic field. These are thought to represent states of high and
  low small-scale magnetic activity of a stellar magnetic cycle. <BR
  /> Results: We find that the presence of small-scale magnetism
  increases the bolometric intensity and flux in all investigated
  models. The surplus in radiative flux of the magnetic over the magnetic
  field-free atmosphere increases with increasing effective temperature,
  T<SUB>eff</SUB>, from 0.47% for spectral type K8V to 1.05% for the solar
  model, but decreases for higher effective temperatures than solar. The
  degree of evacuation of the magnetic flux concentrations monotonically
  increases with T<SUB>eff</SUB> as does their depression of the visible
  optical surface, that is the Wilson depression. Nevertheless, the
  strength of the field concentrations on this surface stays remarkably
  unchanged at ≈1560 G throughout the considered range of spectral
  types. With respect to the surrounding gas pressure, the field strength
  is close to (thermal) equipartition for the Sun and spectral type F5V
  but is clearly sub-equipartition for K2V and more so for K8V. The
  magnetic flux concentrations appear most conspicuous for model K2V
  owing to their high brightness contrast. <BR /> Conclusions: For mean
  magnetic flux densities of approximately 50 G, we expect the small-scale
  magnetism of stars in the spectral range from F5V to K8V to produce a
  positive contribution to their bolometric luminosity. The modulation
  seems to be most effective for early G-type stars.

---------------------------------------------------------
Title: Using the CIFIST grid of CO<SUP>5</SUP>BOLD 3D model
    atmospheres to study the effects of stellar granulation on photometric
    colours. II. The role of convection across the H-R diagram
Authors: Kučinskas, A.; Klevas, J.; Ludwig, H. -G.; Bonifacio, P.;
   Steffen, M.; Caffau, E.
2018A&A...613A..24K    Altcode: 2018arXiv180200073K
  <BR /> Aims: We studied the influence of convection on the spectral
  energy distributions (SEDs), photometric magnitudes, and colour
  indices of different types of stars across the H-R diagram. <BR />
  Methods: The 3D hydrodynamical CO<SUP>5</SUP>BOLD, averaged ⟨3D⟩,
  and 1D hydrostatic LHD model atmospheres were used to compute SEDs
  of stars on the main sequence (MS), main sequence turn-off (TO),
  subgiant branch (SGB), and red giant branch (RGB), in each case at
  two different effective temperatures and two metallicities, [M/H] =
  0.0 and - 2.0. Using the obtained SEDs, we calculated photometric
  magnitudes and colour indices in the broad-band Johnson-Cousins
  UBVRI and 2MASS JHK<SUB>s</SUB>, and the medium-band Strömgren
  uvby photometric systems. <BR /> Results: The 3D-1D differences in
  photometric magnitudes and colour indices are small in both photometric
  systems and typically do not exceed ± 0.03 mag. Only in the case of the
  coolest giants located on the upper RGB are the differences in the U and
  u bands able reach ≈-0.2 mag at [M/H] = 0.0 and ≈-0.1 mag at [M/H]
  = -2.0. Generally, the 3D-1D differences are largest in the blue-UV
  part of the spectrum and decrease towards longer wavelengths. They
  are also sensitive to the effective temperature and are significantly
  smaller in hotter stars. Metallicity also plays a role and leads to
  slightly larger 3D-1D differences at [M/H] = 0.0. All these patterns are
  caused by a complex interplay between the radiation field, opacities,
  and horizontal temperature fluctuations that occur due to convective
  motions in stellar atmospheres. Although small, the 3D-1D differences
  in the magnitudes and colour indices are nevertheless comparable to
  or larger than typical photometric uncertainties and may therefore
  cause non-negligible systematic differences in the estimated effective
  temperatures.

---------------------------------------------------------
Title: TOPoS. IV. Chemical abundances from high-resolution
    observations of seven extremely metal-poor stars
Authors: Bonifacio, P.; Caffau, E.; Spite, M.; Spite, F.; Sbordone,
   L.; Monaco, L.; François, P.; Plez, B.; Molaro, P.; Gallagher, A. J.;
   Cayrel, R.; Christlieb, N.; Klessen, R. S.; Koch, A.; Ludwig, H. -G.;
   Steffen, M.; Zaggia, S.; Abate, C.
2018A&A...612A..65B    Altcode: 2018arXiv180103935B
  Context. Extremely metal-poor (EMP) stars provide us with indirect
  information on the first generations of massive stars. The TOPoS
  survey has been designed to increase the census of these stars and to
  provide a chemical inventory that is as detailed as possible. <BR />
  Aims: Seven of the most iron-poor stars have been observed with the
  UVES spectrograph at the ESO VLT Kueyen 8.2 m telescope to refine
  their chemical composition. <BR /> Methods: We analysed the spectra
  based on 1D LTE model atmospheres, but also used 3D hydrodynamical
  simulations of stellar atmospheres. <BR /> Results: We measured carbon
  in six of the seven stars: all are carbon-enhanced and belong to the
  low-carbon band, defined in the TOPoS II paper. We measured lithium
  (A(Li) = 1.9) in the most iron-poor star (SDSS J1035+0641, [Fe/H]
  &lt;-5.2). We were also able to measure Li in three stars at [Fe/H]
  -4.0, two of which lie on the Spite plateau. We confirm that SDSS
  J1349+1407 is extremely rich in Mg, but not in Ca. It is also very
  rich in Na. Several of our stars are characterised by low α-to-iron
  ratios. <BR /> Conclusions: The lack of high-carbon band stars at low
  metallicity can be understood in terms of evolutionary timescales
  of binary systems. The detection of Li in SDSS J1035+0641 places a
  strong constraint on theories that aim at solving the cosmological
  lithium problem. The Li abundance of the two warmer stars at [Fe/H]
  -4.0 places them on the Spite plateau, while the third, cooler star,
  lies below. We argue that this suggests that the temperature at which
  Li depletion begins increases with decreasing [Fe/H]. SDSS J1349+1407
  may belong to a class of Mg-rich EMP stars. We cannot assess if there
  is a scatter in α-to-iron ratios among the EMP stars or if there are
  several discrete populations. However, the existence of stars with
  low α-to-iron ratios is supported by our observations. <P />Based
  on observations obtained at ESO Paranal Observatory, Programmes
  189.D-0165,090.D-0306, 093.D-0136, and 096.D-0468.

---------------------------------------------------------
Title: PEPSI deep spectra. I. The Sun-as-a-star
Authors: Strassmeier, K. G.; Ilyin, I.; Steffen, M.
2018A&A...612A..44S    Altcode: 2017arXiv171206960S
  Context. Full-disk solar flux spectra can be directly compared to
  stellar spectra and thereby serve as our most important reference
  source for, for example stellar chemical abundances, magnetic activity
  phenomena, radial-velocity signatures or global pulsations. Aim. As part
  of the first Potsdam Echelle Polarimetric and Spectroscopic Instrument
  (PEPSI) key-science project, we aim to provide well-exposed and
  average-combined (viz. deep) high-resolution spectra of representative
  stellar targets. Such deep spectra contain an overwhelming amount
  of information, typically much more than what could be analyzed and
  discussed within a single publication. Therefore, these spectra will
  be made available in form of (electronic) atlases. The first star in
  this series of papers is our Sun. It also acts as a system-performance
  cornerstone. <BR /> Methods: The Sun was monitored with PEPSI at the
  Large Binocular Telescope (LBT). Instead of the LBT we used a small
  robotic solar disk integration (SDI) telescope. The deep spectra
  in this paper are the results of combining up to ≈100 consecutive
  exposures per wavelength setting and are compared with other solar
  flux atlases. <BR /> Results: Our software for the optimal data
  extraction and reduction of PEPSI spectra is described and verified
  with the solar data. Three deep solar flux spectra with a spectral
  resolution of up to 270 000, a continuous wavelength coverage from
  383 nm to 914 nm, and a photon signal to noise ratio (S/N) of between
  2000-8000:1 depending on wavelength are presented. Additionally,
  a time-series of 996 high-cadence spectra in one cross disperser
  is used to search for intrinsic solar modulations. The wavelength
  calibration based on Th-Ar exposures and simultaneous Fabry-Pérot
  combs enables an absolute wavelength solution within 10 m s<SUP>-1</SUP>
  (rms) with respect to the HARPS laser-comb solar atlas and a relative
  rms of 1.2 m s<SUP>-1</SUP> for one day. For science demonstration,
  we redetermined the disk-average solar Li abundance to 1.09 ±
  0.04 dex on the basis of 3D NLTE model atmospheres. We detected
  disk-averaged p-mode RV oscillations with a full amplitude of
  47 cm s<SUP>-1</SUP> at 5.5 min. <BR /> Conclusions: Comparisons
  with two solar FTS atlases, as well as with the HARPS solar atlas,
  validate the PEPSI data product. Now, PEPSI/SDI solar-flux spectra
  are being taken with a sampling of one deep spectrum per day, and
  are supposed to continue a full magnetic cycle of the Sun. <P />Based
  on data acquired with PEPSI fed by the solar disk integration (SDI)
  telescope operated by AIP at the Large Binocular Telescope Observatory
  (LBTO). The LBT is an international collaboration among institutions
  in the United States, Italy and Germany. LBT Corporation partners are:
  The University of Arizona on behalf of the Arizona Board of Regents;
  Istituto Nazionale di Astrofisica, Italy; LBT Beteiligungsgesellschaft,
  Germany, representing the Max-Planck Society, The Leibniz Institute for
  Astrophysics Potsdam (AIP), and Heidelberg University; The Ohio State
  University, and The Research Corporation, on behalf of The University
  of Notre Dame, University of Minnesota and University of Virginia.

---------------------------------------------------------
Title: Using the CIFIST grid of CO<SUP>5</SUP>BOLD 3D model
    atmospheres to study the effects of stellar granulation on photometric
    colours. I. Grids of 3D corrections in the UBVRI, 2MASS, HIPPARCOS,
    Gaia, and SDSS systems
Authors: Bonifacio, P.; Caffau, E.; Ludwig, H. -G.; Steffen, M.;
   Castelli, F.; Gallagher, A. J.; Kučinskas, A.; Prakapavičius, D.;
   Cayrel, R.; Freytag, B.; Plez, B.; Homeier, D.
2018A&A...611A..68B    Altcode: 2017arXiv171200024B
  Context. The atmospheres of cool stars are temporally and spatially
  inhomogeneous due to the effects of convection. The influence of
  this inhomogeneity, referred to as granulation, on colours has never
  been investigated over a large range of effective temperatures and
  gravities. Aim. We aim to study, in a quantitative way, the impact of
  granulation on colours. <BR /> Methods: We use the CIFIST (Cosmological
  Impact of the FIrst Stars) grid of CO5BOLD (COnservative COde for the
  COmputation of COmpressible COnvection in a BOx of L Dimensions, L = 2,
  3) hydrodynamical models to compute emerging fluxes. These in turn are
  used to compute theoretical colours in the UBV RI, 2MASS, HIPPARCOS,
  Gaia and SDSS systems. Every CO5BOLD model has a corresponding one
  dimensional (1D) plane-parallel LHD (Lagrangian HydroDynamics) model
  computed for the same atmospheric parameters, which we used to define
  a "3D correction" that can be applied to colours computed from fluxes
  computed from any 1D model atmosphere code. As an example, we illustrate
  these corrections applied to colours computed from ATLAS models. <BR />
  Results: The 3D corrections on colours are generally small, of the order
  of a few hundredths of a magnitude, yet they are far from negligible. We
  find that ignoring granulation effects can lead to underestimation of
  Teff by up to 200 K and overestimation of gravity by up to 0.5 dex, when
  using colours as diagnostics. We have identified a major shortcoming in
  how scattering is treated in the current version of the CIFIST grid,
  which could lead to offsets of the order 0.01 mag, especially for
  colours involving blue and UV bands. We have investigated the Gaia and
  HIPPARCOS photometric systems and found that the (G - H<SUB>p</SUB>),
  (BP - RP) diagram is immune to the effects of granulation. In addition,
  we point to the potential of the RVS photometry as a metallicity
  diagnostic. <BR /> Conclusions: Our investigation shows that the
  effects of granulation should not be neglected if one wants to use
  colours as diagnostics of the stellar parameters of F, G, K stars. A
  limitation is that scattering is treated as true absorption in our
  current computations, thus our 3D corrections are likely an upper
  limit to the true effect. We are already computing the next generation
  of the CIFIST grid, using an approximate treatment of scattering. <P
  />The appendix tables are only available at the CDS via anonymous ftp
  to <A href="http://cdsarc.u-strasbg.fr">http://cdsarc.u-strasbg.fr</A>
  (<A href="http://cdsarc.u-strasbg.fr">http://130.79.128.5</A>) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/611/A68">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/611/A68</A>

---------------------------------------------------------
Title: VizieR Online Data Catalog: 3D correction in 5 photometric
    systems (Bonifacio+, 2018)
Authors: Bonifacio, P.; Caffau, E.; Ludwig, H. -G.; Steffen, M.;
   Castelli, F.; Gallagher, A. J.; Kucinskas, A.; Prakapavicius, D.;
   Cayrel, R.; Freytag, B.; Plez, B.; Homeier, D.
2018yCat..36110068B    Altcode:
  We have used the CIFIST grid of CO5BOLD models to investigate the
  effects of granulation on fluxes and colours of stars of spectral
  type F, G, and K. <P />We publish tables with 3D corrections that
  can be applied to colours computed from any 1D model atmosphere. For
  Teff&gt;=5000K, the corrections are smooth enough, as a function
  of atmospheric parameters, that it is possible to interpolate the
  corrections between grid points; thus the coarseness of the CIFIST
  grid should not be a major limitation. However at the cool end there
  are still far too few models to allow a reliable interpolation. <P
  />(20 data files).

---------------------------------------------------------
Title: Analysis of the X-ray spectrum of the hot bubble of BD+30°3639
Authors: Schönberner, Detlef; Jacob, Ralf; Heller, René; Steffen,
   Matthias
2017IAUS..323..109S    Altcode: 2016arXiv161201389S
  We developed a model for wind-blown bubbles with temperature
  and density profiles based on self-similar solutions including
  thermal conduction. We constructed also heat-conduction bubbles with
  chemical discontinuities. The X-ray emission is computed using the
  well-documented CHIANTI code (v6.0.1). These bubble models are used
  to (re)analyse the high-resolution X-ray spectrum of the hot bubble
  of BD+30°3639, and they appeared to be much superior to constant
  temperature approaches. <P />We found for the X-ray emission of
  BD+30°3639 that temperature-sensitive and abundance-sensitive line
  ratios computed on the basis of heat-conducting wind-blown bubbles and
  with abundances as found in the stellar photosphere/wind can only be
  reconciled with the observations if the hot bubble of BD+30°3639 is
  chemically stratified, i.e. if it contains also a small mass fraction
  (~= 3 %) of hydrogen-rich matter immediately behind the conduction
  front. Neon appears to be strongly enriched, with a mass fraction of
  at least about 0.06.

---------------------------------------------------------
Title: The Gaia-ESO Survey: Galactic evolution of sulphur and zinc
Authors: Duffau, S.; Caffau, E.; Sbordone, L.; Bonifacio, P.;
   Andrievsky, S.; Korotin, S.; Babusiaux, C.; Salvadori, S.; Monaco, L.;
   François, P.; Skúladóttir, Á.; Bragaglia, A.; Donati, P.; Spina,
   L.; Gallagher, A. J.; Ludwig, H. -G.; Christlieb, N.; Hansen, C. J.;
   Mott, A.; Steffen, M.; Zaggia, S.; Blanco-Cuaresma, S.; Calura, F.;
   Friel, E.; Jiménez-Esteban, F. M.; Koch, A.; Magrini, L.; Pancino,
   E.; Tang, B.; Tautvaišienė, G.; Vallenari, A.; Hawkins, K.; Gilmore,
   G.; Randich, S.; Feltzing, S.; Bensby, T.; Flaccomio, E.; Smiljanic,
   R.; Bayo, A.; Carraro, G.; Casey, A. R.; Costado, M. T.; Damiani,
   F.; Franciosini, E.; Hourihane, A.; Jofré, P.; Lardo, C.; Lewis,
   J.; Morbidelli, L.; Sousa, S. G.; Worley, C. C.
2017A&A...604A.128D    Altcode: 2017arXiv170402981D
  Context. Due to their volatile nature, when sulphur and zinc are
  observed in external galaxies, their determined abundances represent
  the gas-phase abundances in the interstellar medium. This implies
  that they can be used as tracers of the chemical enrichment of matter
  in the Universe at high redshift. Comparable observations in stars
  are more difficult and, until recently, plagued by small number
  statistics. <BR /> Aims: We wish to exploit the Gaia-ESO Survey
  (GES) data to study the behaviour of sulphur and zinc abundances
  of a large number of Galactic stars, in a homogeneous way. <BR />
  Methods: By using the UVES spectra of the GES sample, we are able to
  assemble a sample of 1301 Galactic stars, including stars in open and
  globular clusters in which both sulphur and zinc were measured. <BR
  /> Results: We confirm the results from the literature that sulphur
  behaves as an α-element. We find a large scatter in [Zn/Fe] ratios
  among giant stars around solar metallicity. The lower ratios are
  observed in giant stars at Galactocentric distances less than 7.5
  kpc. No such effect is observed among dwarf stars, since they do not
  extend to that radius. <BR /> Conclusions: Given the sample selection,
  giants and dwarfs are observed at different Galactic locations, and it
  is plausible, and compatible with simple calculations, that Zn-poor
  giants trace a younger population more polluted by SN Ia yields. It
  is necessary to extend observations in order to observe both giants
  and dwarfs at the same Galactic location. Further theoretical work on
  the evolution of zinc is also necessary. <P />Based on observations
  collected at the European Organisation for Astronomical Research in the
  Southern Hemisphere under ESO programmes 188.B-3002, 193.B-0936.The full
  table of S abundances is only available at the CDS via anonymous ftp
  to <A href="http://cdsarc.u-strasbg.fr">http://cdsarc.u-strasbg.fr</A>
  (<A href="http://130.79.128.5">http://130.79.128.5</A>) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/604/A128">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/604/A128</A>

---------------------------------------------------------
Title: Lithium abundance and <SUP>6</SUP>Li/<SUP>7</SUP>Li ratio in
    the active giant HD 123351. I. A comparative analysis of 3D and 1D
    NLTE line-profile fits
Authors: Mott, A.; Steffen, M.; Caffau, E.; Spada, F.; Strassmeier,
   K. G.
2017A&A...604A..44M    Altcode: 2017arXiv170406460M
  Context. Current three-dimensional (3D) hydrodynamical model
  atmospheres together with detailed spectrum synthesis, accounting
  for departures from local thermodynamic equilibrium (LTE), permit
  to derive reliable atomic and isotopic chemical abundances from
  high-resolution stellar spectra. Not much is known about the presence
  of the fragile <SUP>6</SUP>Li isotope in evolved solar-metallicity red
  giant branch (RGB) stars, not to mention its production in magnetically
  active targets like HD 123351. <BR /> Aims: A detailed spectroscopic
  investigation of the lithium resonance doublet in HD 123351 in terms
  of both abundance and isotopic ratio is presented. From fits of
  the observed spectrum, taken at the Canada-France-Hawaii telescope,
  with synthetic line profiles based on 1D and 3D model atmospheres,
  we seek to estimate the abundance of the <SUP>6</SUP>Li isotope and
  to place constraints on its origin. <BR /> Methods: We derive the
  lithium abundance A(Li) and the <SUP>6</SUP>Li/<SUP>7</SUP>Li isotopic
  ratio by fitting different synthetic spectra to the Li-line region
  of a high-resolution CFHT spectrum (R = 120 000, S/N = 400). The
  synthetic spectra are computed with four different line lists,
  using in parallel 3D hydrodynamical CO<SUP>5</SUP>BOLD and 1D LHD
  model atmospheres and treating the line formation of the lithium
  components in non-LTE (NLTE). The fitting procedure is repeated with
  different assumptions and wavelength ranges to obtain a reasonable
  estimate of the involved uncertainties. <BR /> Results: We find A(Li)
  = 1.69 ± 0.11 dex and <SUP>6</SUP>Li/<SUP>7</SUP>Li = 8.0 ± 4.4%
  in 3D-NLTE, using the line list of Meléndez et al. (2012, A&amp;A,
  543, A29), updated with new atomic data for V I, which results in
  the best fit of the lithium line profile of HD 123351. Two other line
  lists lead to similar results but with inferior fit qualities. <BR />
  Conclusions: Our 2σ detection of the <SUP>6</SUP>Li isotope is the
  result of a careful statistical analysis and the visual inspection
  of each achieved fit. Since the presence of a significant amount of
  <SUP>6</SUP>Li in the atmosphere of a cool evolved star is not expected
  in the framework of standard stellar evolution theory, non-standard,
  external lithium production mechanisms, possibly related to stellar
  activity or a recent accretion of rocky material, need to be invoked
  to explain the detection of <SUP>6</SUP>Li in HD 123351.

---------------------------------------------------------
Title: Abundances of Na, Mg, and K in the atmospheres of red giant
    branch stars of Galactic globular cluster 47 Tucanae
Authors: Černiauskas, A.; Kučinskas, A.; Klevas, J.; Prakapavičius,
   D.; Korotin, S.; Bonifacio, P.; Ludwig, H. -G.; Caffau, E.; Steffen, M.
2017A&A...604A..35C    Altcode: 2017arXiv170402751C
  <BR /> Aims: We study the abundances of Na, Mg, and K in the atmospheres
  of 32 red giant branch (RGB) stars in the Galactic globular cluster
  (GGC) 47 Tuc, with the goal to investigate the possible existence of
  Na-K and Mg-K correlations/anti-correlations, similar to those that
  were recently discovered in two other GGCs, NGC 2419 and 2808. <BR
  /> Methods: The abundances of K, Na, and Mg were determined using
  high-resolution 2dF/HERMES spectra obtained with the Anglo-Australian
  Telescope (AAT). The one-dimensional (1D) NLTE abundance estimates
  were obtained using 1D hydrostatic ATLAS9 model atmospheres and
  spectral line profiles synthesized with the MULTI package. We also
  used three-dimensional (3D) hydrodynamical CO<SUP>5</SUP>BOLD and
  1D hydrostatic LHD model atmospheres to compute 3D-1D LTE abundance
  corrections, Δ<SUB>3D - 1D LTE</SUB>, for the spectral lines of Na,
  Mg, and K used in our study. These abundance corrections were used to
  understand the role of convection in the formation of spectral lines,
  as well as to estimate the differences in the abundances obtained with
  the 3D hydrodynamical and 1D hydrostatic model atmospheres. <BR />
  Results: The average element-to-iron abundance ratios and their RMS
  variations due to star-to-star abundance spreads determined in our
  sample of RGB stars were ⟨ [ Na / Fe ] ⟩ <SUP>1D NLTE</SUP> =
  0.42 ± 0.13, ⟨ [ Mg / Fe ] ⟩ <SUP>1D NLTE</SUP> = 0.41 ± 0.11,
  and ⟨ [ K / Fe ] ⟩ <SUP>1D NLTE</SUP> = 0.05 ± 0.14. We found no
  statistically significant relations between the abundances of the three
  elements studied here. Also, there were no abundance trends with the
  distance from the cluster center, nor any statistically significant
  relations between the abundance/abundance ratios and absolute radial
  velocities of individual stars. All these facts suggest the similarity
  of K abundance in stars that belong to different generations in 47
  Tuc which, in turn, may hint that evolution of K in this particular
  cluster was unrelated to the nucleosynthesis of Na and/or Mg.

---------------------------------------------------------
Title: VizieR Online Data Catalog: S abundances for 1301 stars from
    GES (Duffau+, 2017)
Authors: Duffau, S.; Caffau, E.; Sbordone, L.; Bonifacio, P.;
   Andrievsky, S.; Korotin, S.; Babusiaux, C.; Salvadori, S.; Monaco,
   L.; Francois, P.; Skuladottir, A.; Bragaglia, A.; Donati, P.; Spina,
   L.; Gallagher, A. J.; Ludwig, H. -G.; Christlieb, N.; Hansen, C. J.;
   Mott, A.; Steffen, M.; Zaggia, S.; Blanco-Cuaresma, S.; Calura, F.;
   Friel, E.; Jimenez-Esteban, F. M.; Koch, A.; Magrini, L.; Pancino,
   E.; Tang, B.; Tautvaisiene, G.; Vallenari, A.; Hawkins, K.; Gilmore,
   G.; Randich, S.; Feltzing, S.; Bensby, T.; Flaccomio, E.; Smiljanic,
   R.; Bayo, A.; Carraro, G.; Casey, A. R.; Costado, M. T.; Damiani,
   F.; Franciosini, E.; Hourihane, A.; Jofre, P.; Lardo, C.; Lewis, J.;
   Morbidelli, L.; Sousa, S. G.; Worley, C. C.
2017yCat..36040128D    Altcode:
  GES internal star identifier (CNAME), Sulphur abundances and NLTE
  corrections to the Sulphur abundances for 1301 stars. Sulphur
  abundances are expressed in the customary logarithmic form:
  A(S)=log_10(N(S)/N(H))+12. The abundances delivered are the LTE
  ones. NLTEabundances can be determined by directly summing the NLTE
  correction delivered: A(S)<SUB>NLTE = A(S) + NLTE</SUB>C. So that a
  negative NLTE correction indicates that the NLTE abundance is lower
  than the LTE one. <P />(1 data file).

---------------------------------------------------------
Title: Three-dimensional hydrodynamical CO<SUP>5</SUP>BOLD model
    atmospheres of red giant stars. V. Oxygen abundance in the metal-poor
    giant HD 122563 from OH UV lines
Authors: Prakapavičius, D.; Kučinskas, A.; Dobrovolskas, V.; Klevas,
   J.; Steffen, M.; Bonifacio, P.; Ludwig, H. -G.; Spite, M.
2017A&A...599A.128P    Altcode: 2016arXiv161103283P
  Context. Although oxygen is an important tracer of the early Galactic
  evolution, its abundance trends with metallicity are still relatively
  poorly known at [Fe/H] ≲ -2.5. This is in part due to a lack of
  reliable oxygen abundance indicators in the metal-poor stars, and in
  part due to shortcomings in 1D LTE abundance analyses where different
  abundance indicators, such as OH lines located in the UV and IR or
  the forbidden [O I] line at 630 nm, frequently provide inconsistent
  results. <BR /> Aims: In this study, we determined the oxygen abundance
  in the metal-poor halo giant HD 122563 using a 3D hydrodynamical
  CO<SUP>5</SUP>BOLD model atmosphere. Our main goal was to understand
  whether a 3D LTE analysis can help to improve the reliability of oxygen
  abundances that are determined from OH UV lines in comparison to those
  obtained using standard 1D LTE methodology. <BR /> Methods: The oxygen
  abundance in HD 122563 was determined using 71 OH UV lines located in
  the wavelength range between 308-330 nm. The analysis was performed
  using a high-resolution VLT UVES spectrum with a 1D LTE spectral line
  synthesis performed using the SYNTHE package and classical ATLAS9
  model atmosphere. Subsequently, a 3D hydrodynamical CO<SUP>5</SUP>BOLD
  and 1D hydrostatic LHD model atmospheres were used to compute 3D-1D
  abundance corrections. For this, the microturbulence velocity used
  with the 1D LHD model atmosphere was derived from the hydrodynamical
  CO<SUP>5</SUP>BOLD model atmosphere of HD 122563. The obtained abundance
  corrections were then applied to determine 3D LTE oxygen abundances from
  each individual OH UV line. <BR /> Results: As in previous studies,
  we found trends in the 1D LTE oxygen abundances determined from OH UV
  lines with line parameters, such as the line excitation potential, χ,
  and the line equivalent width, W. These trends become significantly less
  pronounced in 3D LTE. Using OH UV lines, we determined a 3D LTE oxygen
  abundance in HD 122563 of A(O)<SUB>3D LTE</SUB> = 6.23 ± 0.13 ([O/Fe]
  = 0.07 ± 0.13). This is in fair agreement with the oxygen abundance
  obtained from OH IR lines, A(O)<SUB>3D LTE</SUB> = 6.39 ± 0.11 ([O/Fe]
  = 0.23 ± 0.11), but it is noticeably lower than that determined when
  using the forbidden [O I] line, A(O)<SUB>3D LTE</SUB> = 6.53 ± 0.15
  ([O/Fe] = 0.37 ± 0.15). While the exact cause of this discrepancy
  remains unclear, it is very likely that non-LTE effects may play a
  decisive role here. Oxygen-to-iron ratios determined in HD 122563
  using OH UV/IR lines and the forbidden [O I] line fall on the lower
  boundary of the [O/Fe] distribution as observed in the Galactic field
  stars at this metallicity and suggest a very mild oxygen overabundance
  with respect to iron, [O/Fe] ≲ 0.4.

---------------------------------------------------------
Title: VizieR Online Data Catalog: NGC104 RGB Na, Mg, and K abundances
    (Cerniauskas+, 2017)
Authors: Cerniauskas, A.; Kucinskas, A.; Klevas, J.; Prakapavicius,
   D.; Korotin, S.; Bonifacio, P.; Ludwig, H. -G.; Caffau, E.; Steffen, M.
2017yCat..36040035C    Altcode:
  We used 2dF/HERMES spectra obtained in two wavelength regions,
  564.9-587.3nm (GREEN) and 758.5-788.7nm (IR), using the spectral
  resolution of R~28000 and exposure time of 1200s. The observations
  were carried out during the period of Oct 22 - Dec 20, 2013 <P />(1
  data file).

---------------------------------------------------------
Title: An in-depth spectroscopic examination of molecular bands from
    3D hydrodynamical model atmospheres. II. Carbon-enhanced metal-poor
    3D model atmospheres
Authors: Gallagher, A. J.; Caffau, E.; Bonifacio, P.; Ludwig, H. -G.;
   Steffen, M.; Homeier, D.; Plez, B.
2017A&A...598L..10G    Altcode: 2017arXiv170109102G
  Context. Tighter constraints on metal-poor stars we observe are
  needed to better understand the chemical processes of the early
  Universe. Computing a stellar spectrum in 3D allows one to model complex
  stellar behaviours, which cannot be replicated in 1D. <BR /> Aims:
  We examine the effect that the intrinsic CNO abundances have on a 3D
  model structure and the resulting 3D spectrum synthesis. <BR /> Methods:
  Model atmospheres were computed in 3D for three distinct CNO chemical
  compositions using the CO<SUP>5</SUP>BOLD model atmosphere code,
  and their internal structures were examined. Synthetic spectra were
  computed from these models using Linfor3D and they were compared. New
  3D abundance corrections for the G-band and a selection of UV OH lines
  were also computed. <BR /> Results: The varying CNO abundances change
  the metal content of the 3D models. This had an effect on the model
  structure and the resulting synthesis. However, it was found that
  the C/O ratio had a larger effect than the overall metal content of
  a model. <BR /> Conclusions: Our results suggest that varying the
  C/O ratio has a substantial impact on the internal structure of the
  3D model, even in the hot turn-off star models explored here. This
  suggests that bespoke 3D models, for specific CNO abundances should
  be sought. Such effects are not seen in 1D at these temperature regimes.

---------------------------------------------------------
Title: 3D non-LTE corrections for the <SUP>6</SUP>Li/<SUP>7</SUP>Li
    isotopic ratio in solar-type stars
Authors: Harutyunyan, G.; Steffen, M.; Mott, A.; Caffau, E.; Israelian,
   G.; González Hernández, J. I.; Strassmeier, K. G.
2017MmSAI..88...61H    Altcode:
  Doppler shifts induced by convective motions in stellar atmospheres
  affect the shape of spectral absorption lines and create slightly
  asymmetric line profiles. It is important to take this effect into
  account in modeling the subtle depression created by the <SUP>6</SUP>Li
  isotope which lies on the red wing of the Li I 670.8 nm resonance
  doublet line, since convective motions in stellar atmospheres can mimic
  a presence of <SUP>6</SUP>Li when intrinsically symmetric theoretical
  line profiles are presumed for the analysis of the <SUP>7</SUP>Li
  doublet \citep{cayrel2007}. Based on CO5BOLD hydrodynamical model
  atmospheres, we compute 3D non-local thermodynamic equilibrium
  (NLTE) corrections for the <SUP>6</SUP>Li/<SUP>7</SUP>Li isotopic
  ratio by using a grid of 3D NLTE and 1D LTE synthetic spectra. These
  corrections must be added to the results of the 1D LTE analysis to
  correct them for the combined 3D non-LTE effects. As one would expect,
  the resulting corrections are always negative and they range between
  0 and -5 %, depending on effective temperature, surface gravity, and
  metallicity. For each metallicity we derive an analytic expression
  approximating the 3D NLTE corrections as a function of effective
  temperature, surface gravity and projected rotational velocity.

---------------------------------------------------------
Title: Radiation transport in CO5BOLD. A short-characteristics module
    for local box models
Authors: Steffen, M.
2017MmSAI..88...22S    Altcode:
  We give a description of a new radiative transfer package based on an
  energy-conserving short-characteristics (SC) approach, developed for
  both CO5BOLD 3D radiation hydrodynamics local box simulations and NLTE3D
  line formation post processing. First test results for a realistic 3D
  solar atmosphere model indicate that the thermal structure obtained
  with the new radiation transport scheme closely matches the one found
  with the standard long-characteristics Feautrier (LCF) method that has
  served in CO5BOLD for many years. This is a very reassuring result,
  corroborating the validity of the CO5BOLD models computed previously
  with the LCF radiation transport.

---------------------------------------------------------
Title: Using CO5BOLD models to predict the effects of granulation
    on colours .
Authors: Bonifacio, P.; Caffau, E.; Ludwig, H. -G.; Steffen, M.;
   Castelli, F.; Gallagher, A. J.; Prakapavičius, D.; Kučinskas, A.;
   Cayrel, R.; Freytag, B.; Plez, B.; Homeier, D.
2017MmSAI..88...90B    Altcode:
  In order to investigate the effects of granulation on fluxes and
  colours, we computed the emerging fluxes from the models in the
  CO5BOLD grid with metallicities [M/H]=0.0,-1.0,-2.0 and -3.0. These
  fluxes have been used to compute colours in different photometric
  systems. We explain here how our computations have been performed and
  provide some results.

---------------------------------------------------------
Title: Enhanced methods for computing spectra from CO5BOLD models
    using Linfor3D. Molecular bands in metal-poor stars
Authors: Gallagher, A. J.; Steffen, M.; Caffau, E.; Bonifacio, P.;
   Ludwig, H. -G.; Freytag, B.
2017MmSAI..88...82G    Altcode: 2016arXiv161004427G
  Molecular features such as the G-band, CN-band and NH-band are important
  diagnostics for measuring a star's carbon and nitrogen abundances,
  especially in metal-poor stars where atomic lines are no longer visible
  in stellar spectra. Unlike atomic transitions, molecular features
  tend to form in bands, which cover large wavelength regions in a
  spectrum. While it is a trivial matter to compute carbon and nitrogen
  molecular bands under the assumption of 1D, it is extremely time
  consuming in 3D. In this contribution to the 2016 COBOLD workshop we
  review the improvements made to the 3D spectral synthesis code Linfor3D,
  and discuss the new challenges found when computing molecular features
  in 3D.

---------------------------------------------------------
Title: Lithium in the active sub-giant HD123351. A quantitative
    analysis with 3D and 1D model atmospheres using different observed
    spectra
Authors: Mott, A.; Steffen, M.; Caffau, E.; Strassmeier, K. G.
2017MmSAI..88...68M    Altcode:
  Current 3D hydrodynamical model atmosphere simulations together with
  non-LTE spectrum synthesis calculations permit to determine reliable
  atomic and in particular isotopic chemical abundances. Although this
  approach is computationally time demanding, it became feasible in
  studying lithium in stellar spectra. In the literature not much is
  known about the presence of the more fragile {<SUP>6</SUP>Li} isotope
  in evolved metal-rich objects. In this case the analysis is complicated
  by the lack of a suitable list of atomic and molecular lines in the
  spectral region of the lithium resonance line at 670.8 nm. <P />Here we
  present a spectroscopic comparative analysis of the Li doublet region
  of HD 123351, an active sub-giant star of solar metallicity. We fit
  the Li profile in three observed spectra characterized by different
  qualities: two very-high resolution spectra (Gecko@CFHT, R=120 000,
  SNR=400 and PEPSI@LBT, R=150 000, SNR=663) and a high-resolution
  SOPHIE@OHP spectrum (R=40 000, SNR=300). We adopt a set of model
  atmospheres, both 3D and 1D, having different stellar parameters
  (T_{eff} and log g). The 3D models are taken from the CIFIST grid of
  COBOLD model atmospheres and departures from LTE are considered for
  the lithium components. For the blends other than the lithium in this
  wavelength region we adopt the linelist of \citet{melendez12}. We find
  consistent results for all three observations and an overall good fit
  with the selected list of atomic and molecular lines, indicating a
  high {<SUP>6</SUP>Li} content. <P />The presence of {<SUP>6</SUP>Li}
  is not expected in cool stellar atmospheres. Its detection is of
  crucial importance for understanding mixing processes in stars and
  external lithium production mechanisms, possibly related to stellar
  activity or planetray accretion of {<SUP>6</SUP>Li}-rich material.

---------------------------------------------------------
Title: The influence of convection on OH UV line formation in the
    atmosphere of the metal-poor red giant HD 122563.
Authors: Prakapavičius, D.; Kučinskas, A.; Dobrovolskas, V.; Klevas,
   J.; Steffen, M.; Bonifacio, P.; Ludwig, H. -G.; Spite, M.
2017MmSAI..88...77P    Altcode:
  We utilized high-resolution spectra of the metal-poor red giant star
  HD 122563 and classical 1D hydrostatic ATLAS9 model atmosphere to
  derive the 1D LTE oxygen abundance from OH UV lines. The obtained
  average 1D LTE oxygen abundance is xtmean {ensuremath {A(O)_{1D
  LTE}} = 6.41 ± 0.16. We also used 3D hydrodynamical COBOLD and 1D
  hydrostatic LHD model atmospheres to correct the 1D LTE abundances for
  convection-related effects and to determine average 3D LTE abundance,
  xtmean {ensuremath {A(O)_{3D LTE}} = 6.23 ± 0.13. We found that while
  the oxygen abundances determined using 1D hydrostatic model atmospheres
  showed trends both with the line strength and excitation potential,
  these trends essentially disappeared in the 3D LTE case. The average 3D
  LTE oxygen abundance obtained from the OH UV lines agrees reasonably
  well with the oxygen abundances obtained in the earlier analyses from
  the OH IR lines and the 630.0 nm [O I] line, while the remaining small
  discrepancies may possibly be attributed to NLTE effects.

---------------------------------------------------------
Title: Investigation of the solar centre-to-limb variation of oxygen
    and lithium spectral features
Authors: Caffau, E.; Malherbe, J. -M.; Steffen, M.; Ludwig, H. -G.;
   Mott, A.
2017MmSAI..88...45C    Altcode:
  We compare intensity spectra of the Sun observed at different limb
  angles in the wavelength range covering the forbidden oxygen lines and
  the lithium resonance feature with line formation computations performed
  on a CO5BOLD 3D hydrodynamical simulation of the solar atmosphere. Among
  the prime oxygen abundance indicators, the forbidden line at 630 nm
  is contaminated with a significant Ni I blend. The availability of
  observations at different positions on the solar disc allows us to
  disentangle the contributions of oxygen and nickel and to derive their
  individual abundances. We derived in the past, from the [OI] line,
  A(O)=8.73± 0.05 with a nickel abundance of A(Ni)=6.1± 0.04. From
  the observations here presented, we obtain A(O)=8.71 and A(Ni)=6.09,
  in excellent agreement with the previous result. For lithium, we
  investigated the Li doublet at 670.7 nm and compared synthetic spectra
  of the Li spectra range based on different line-lists available in the
  literature to the observed data. With these observations, we are still
  unable to conclude on which is the best line-list to be used for the
  blending lines.

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Title: TOPoS. III. An ultra iron-poor multiple CEMP system
Authors: Caffau, E.; Bonifacio, P.; Spite, M.; Spite, F.; Monaco, L.;
   Sbordone, L.; François, P.; Gallagher, A. J.; Plez, B.; Zaggia, S.;
   Ludwig, H. -G.; Cayrel, R.; Koch, A.; Steffen, M.; Salvadori, S.;
   Klessen, R.; Glover, S.; Christlieb, N.
2016A&A...595L...6C    Altcode: 2016arXiv161004106C
  <BR /> Aims: One of the primary objectives of the TOPoS survey
  is to search for the most metal-poor stars. Our search has led
  to the discovery of one of the most iron-poor objects known, SDSS
  J092912.32+023817.0. This object is a multiple system, in which two
  components are clearly detected in the spectrum. <BR /> Methods:
  We have analysed 16 high-resolution spectra obtained using the UVES
  spectrograph at the ESO 8.2 m VLT telescope to measure radial velocities
  and determine the chemical composition of the system. <BR /> Results:
  Cross correlation of the spectra with a synthetic template yields a
  double-peaked cross-correlation function (CCF) for eight spectra, and
  in one case there is evidence for the presence of a third peak. Chemical
  analysis of the spectrum obtained by averaging all the spectra for which
  the CCF showed a single peak found that the iron abundance is [Fe/H] =
  -4.97. The system is also carbon enhanced with [C/Fe] = +3.91 (A(C) =
  7.44). From the permitted oxygen triplet we determined an upper limit
  for oxygen of [O/Fe] &lt; +3.52 such that C/O &gt; 1.3. We are also
  able to provide more stringent upper limits on the Sr and Ba abundances
  ([Sr/Fe] &lt; +0.70, and [Ba/Fe] &lt; +1.46, respectively). <P />Based
  on observations made with ESO Telescopes at the La Silla Paranal
  Observatory under programme ID 094.D-0488 and 096.D-0616.

---------------------------------------------------------
Title: An in-depth spectroscopic examination of molecular bands from
    3D hydrodynamical model atmospheres. I. Formation of the G-band in
    metal-poor dwarf stars
Authors: Gallagher, A. J.; Caffau, E.; Bonifacio, P.; Ludwig, H. -G.;
   Steffen, M.; Spite, M.
2016A&A...593A..48G    Altcode: 2016arXiv160507215G
  Context. Recent developments in the three-dimensional (3D) spectral
  synthesis code Linfor3D have meant that for the first time, large
  spectral wavelength regions, such as molecular bands, can be synthesised
  with it in a short amount of time. <BR /> Aims: A detailed spectral
  analysis of the synthetic G-band for several dwarf turn-off-type 3D
  atmospheres (5850 ≲ T<SUB>eff</SUB> [ K ] ≲ 6550, 4.0 ≤ log g
  ≤ 4.5, - 3.0 ≤ [Fe/H] ≤-1.0) was conducted, under the assumption
  of local thermodynamic equilibrium. We also examine carbon and oxygen
  molecule formation at various metallicity regimes and discuss the impact
  it has on the G-band. <BR /> Methods: Using a qualitative approach,
  we describe the different behaviours between the 3D atmospheres and
  the traditional one-dimensional (1D) atmospheres and how the different
  physics involved inevitably leads to abundance corrections, which
  differ over varying metallicities. Spectra computed in 1D were fit to
  every 3D spectrum to determine the 3D abundance correction. <BR />
  Results: Early analysis revealed that the CH molecules that make up
  the G-band exhibited an oxygen abundance dependency; a higher oxygen
  abundance leads to weaker CH features. Nitrogen abundances showed zero
  impact to CH formation. The 3D corrections are also stronger at lower
  metallicity. Analysis of the 3D corrections to the G-band allows us to
  assign estimations of the 3D abundance correction to most dwarf stars
  presented in the literature. <BR /> Conclusions: The 3D corrections
  suggest that A(C) in carbon-enhanced metal-poor (CEMP) stars with high
  A(C) would remain unchanged, but would decrease in CEMP stars with lower
  A(C). It was found that the C/O ratio is an important parameter to the
  G-band in 3D. Additional testing confirmed that the C/O ratio is an
  equally important parameter for OH transitions under 3D. This presents
  a clear interrelation between the carbon and oxygen abundances in 3D
  atmospheres through their molecular species, which is not seen in 1D.

---------------------------------------------------------
Title: Hydrodynamical model atmospheres: Their impact on stellar
    spectroscopy and asteroseismology of late-type stars
Authors: Ludwig, H. -G.; Steffen, M.
2016AN....337..844L    Altcode: 2016arXiv160900219L
  Hydrodynamical, i.e. multi-dimensional and time-dependent,
  model atmospheres of late-type stars have reached a high level
  of realism. They are commonly applied in high-fidelity work on
  stellar abundances but also allow the study of processes that
  are not modelled in standard, one-dimensional hydrostatic model
  atmospheres. Here, we discuss two observational aspects that emerge
  from such processes, the photometric granulation background and the
  spectroscopic microturbulence. We use CO5BOLD hydrodynamical model
  atmospheres to characterize the total granular brightness fluctuations
  and characteristic time scale for FGK stars. Emphasis is put on the
  diagnostic potential of the granulation background for constraining
  the fundamental atmospheric parameters. We find a clear metallicity
  dependence of the granulation background. The comparison between
  the model predictions and available observational constraints at
  solar metallicity shows significant differences, that need further
  clarification. Concerning microturbulence, we report on the derivation
  of a theoretical calibration based on CO5BOLD models, which shows
  good correspondence with the measurements for stars in the Hyades. We
  emphasize the importance of a consistent procedure when determining
  the microturbulence, and point to limitations of the commonly applied
  description of microturbulence in hydrostatic model atmospheres.

---------------------------------------------------------
Title: Reconstructing the Milky Way's history: spectroscopic surveys,
    asteroseismology, and chemodynamical models
Authors: Chiappini, Cristina; Montalbán, Josefina; Steffen, Matthias
2016AN....337..773C    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Investigation of the lithium 670.7 nm wavelength range in
    the solar spectrum
Authors: Caffau, Elisabetta; Mott, Alessandro; Harutyunyan, Gohar;
   Malherbe, Jean-Marie; Steffen, Matthias
2016cosp...41E.281C    Altcode:
  Lithium is a key chemical element, with a chemical evolution that is
  different from that of most other elements. It is also very fragile,
  as it is destroyed by nuclear reactions with protons at temperatures
  higher than about 2.5 million K. According to standard Big Bang
  nucleosynthesis, only the isotope 7Li is produced in significant
  amounts, while the primordial abundance of the lighter isotope 6Li
  is negligible. Lithium is not produced by nucleosynthesis in normal
  stars, except in peculiar phases of stellar evolution (e.g. in AGB
  stars and Novae). Lithium may also be formed as a result of flares in
  the atmospheres of young, active stars. To investigate the history
  of Li production and depletion in the Galaxy, it is necessary to
  analyse stars of all ages, including those at solar metallicity. In
  this case, the spectroscopic determination of the Li abundance is
  complicated by the presence of other spectral lines overlapping
  with the Li doublet at 670.7 nm. The correct identification and
  knowledge of the atomic parameters of these blend lines is critical,
  especially if the 6LI/7Li isotopic ratio is to be derived. In this
  investigation, we consider several line lists of the blending components
  available in the literature and use them to compute synthetic spectra,
  performing the line formation computations both for the classical 1D
  Holweger-Mueller model and a CO5BOLD 3D hydrodynamical simulation of the
  solar atmosphere. The synthetic spectra are then compared to the solar
  spectrum observed at different limb angles. This allows us to check the
  quality of existing line lists, to find potentially misidentified blend
  lines, and to construct an optimized line list for solar-type stars.

---------------------------------------------------------
Title: The Central Role of FORS1/2 Spectropolarimetric Observations
    for the Progress of Stellar Magnetism Studies
Authors: Schöller, M.; Hubrig, S.; Ilyin, I.; Steffen, M.; Briquet,
   M.; Kholtygin, A. F.
2016Msngr.163...21S    Altcode:
  The spectropolarimetric mode of the FOcal Reducer and low dispersion
  Spectrographs (FORS), which was first implemented in FORS1, and then
  moved to FORS2 seven years ago, has made it possible to probe the
  presence of magnetic fields in stars of different spectral classes
  at almost all stages of stellar evolution. While in the early days of
  FORS1, many of the observations were related to magnetic Ap/Bp stars
  and their progenitor Herbig Ae/Be stars, recent spectropolarimetric
  studies with FORS2 have involved more challenging targets, such as
  massive O- and B-type stars in clusters and in the field, very fast
  rotating massive stars with magnetospheres, Wolf-Rayet stars and
  central stars of planetary nebulae. The role of FORS observations for
  stellar magnetic field measurements is summarised and improvements in
  the measurement technique are described.

---------------------------------------------------------
Title: Hot bubbles of planetary nebulae with hydrogen-deficient
    winds. I. Heat conduction in a chemically stratified plasma
Authors: Sandin, C.; Steffen, M.; Schönberner, D.; Rühling, U.
2016A&A...586A..57S    Altcode: 2015arXiv151204986S
  Heat conduction has been found a plausible solution to explain
  discrepancies between expected and measured temperatures in hot bubbles
  of planetary nebulae (PNe). While the heat conduction process depends
  on the chemical composition, to date it has been exclusively studied
  for pure hydrogen plasmas in PNe. A smaller population of PNe show
  hydrogen-deficient and helium- and carbon-enriched surfaces surrounded
  by bubbles of the same composition; considerable differences are
  expected in physical properties of these objects in comparison to
  the pure hydrogen case. The aim of this study is to explore how
  a chemistry-dependent formulation of the heat conduction affects
  physical properties and how it affects the X-ray emission from PN
  bubbles of hydrogen-deficient stars. We extend the description of
  heat conduction in our radiation hydrodynamics code to work with
  any chemical composition. We then compare the bubble-formation
  process with a representative PN model using both the new and the
  old descriptions. We also compare differences in the resulting X-ray
  temperature and luminosity observables of the two descriptions. The
  improved equations show that the heat conduction in our representative
  model of a hydrogen-deficient PN is nearly as efficient with the
  chemistry-dependent description; a lower value on the diffusion
  coefficient is compensated by a slightly steeper temperature
  gradient. The bubble becomes somewhat hotter with the improved
  equations, but differences are otherwise minute. The observable
  properties of the bubble in terms of the X-ray temperature and
  luminosity are seemingly unaffected.

---------------------------------------------------------
Title: Lithium spectral line formation in stellar atmospheres. The
    impact of convection and NLTE effects
Authors: Klevas, J.; Kučinskas, A.; Steffen, M.; Caffau, E.; Ludwig,
   H. -G.
2016A&A...586A.156K    Altcode: 2015arXiv151208999K
  <BR /> Aims: Because of the complexities involved in treating
  spectral line formation in full 3D and non-local thermodynamic
  equilibrium (NLTE), different simplified approaches are sometimes
  used to account for the NLTE effects with 3D hydrodynamical model
  atmospheres. In certain cases, chemical abundances are derived in
  1D NLTE and then corrected for the 3D effects by adding 3D-1D LTE
  (Local Thermodynamic Equilibrium, LTE) abundance corrections (3D+NLTE
  approach). Alternatively, average ⟨3D⟩ model atmospheres are
  sometimes used to substitute for the full 3D hydrodynamical models. <BR
  /> Methods: In this work we tested whether the results obtained using
  these simplified schemes (3D+NLTE, ⟨3D⟩ NLTE) may reproduce those
  derived using the full 3D NLTE computations. The tests were made using
  3D hydrodynamical CO<SUP>5</SUP>BOLD model atmospheres of the main
  sequence (MS), main sequence turn-off (TO), subgiant (SGB), and red
  giant branch (RGB) stars, all at two metallicities, [ M / H ] = 0.0
  and -2.0. Our goal was to investigate the role of 3D and NLTE effects
  on the formation of the 670.8 nm lithium resonance line. This was done
  by assessing differences in the strengths of synthetic 670.8 nm line
  profiles, which were computed using 3D/1D NLTE/LTE approaches. <BR />
  Results: Our results show that Li 670.8 nm line strengths obtained
  using different methodologies differ only slightly in most of the
  models at solar metallicity studied here. However, the line strengths
  predicted with the 3D NLTE and 3D+NLTE approaches become significantly
  different at subsolar metallicities. At [ M / H ] = -2.0, this may lead
  to (3D NLTE) - (3D+NLTE) differences in the predicted lithium abundance
  of ~0.46 and ~0.31 dex in the TO and RGB stars respectively. On the
  other hand, NLTE line strengths computed with the average ⟨3D⟩ and
  1D model atmospheres are similar to those obtained with the full 3D
  NLTE approach for MS, TO, SGB, and RGB stars, at all metallicities;
  3D - ⟨3D⟩ and 3D - 1D differences in the predicted abundances
  are always less than ~0.04 dex and ~0.08 dex, respectively. However,
  neither of the simplified approaches can reliably substitute 3D NLTE
  spectral synthesis when precision is required.

---------------------------------------------------------
Title: Consistent metallicity scale for cool dwarfs and giants. A
    benchmark test using the Hyades
Authors: Dutra-Ferreira, L.; Pasquini, L.; Smiljanic, R.; Porto de
   Mello, G. F.; Steffen, M.
2016A&A...585A..75D    Altcode: 2015arXiv150907725D
  Context. In several instances chemical abundances of main-sequence
  and giant stars are used simultaneously under the assumption that they
  share the same abundance scale. This assumption, if wrong, might have
  important implications in different astrophysical contexts. <BR />
  Aims: It is therefore crucial to understand whether the metallicity
  or abundance differences among dwarfs and giants are real or are
  produced by systematic errors in the analysis. We aim to ascertain
  a methodology capable of producing a consistent metallicity scale
  for giants and dwarfs. <BR /> Methods: To achieve that, we analyzed
  giants and dwarfs in the Hyades open cluster, under the assumption
  that they share the same chemical composition. All the stars in this
  cluster have archival high-resolution spectroscopic data obtained
  with HARPS and UVES. In addition, the giants have interferometric
  measurements of the angular diameters. We analyzed the sample with
  two methods. The first method constrains the atmospheric parameters
  independently from spectroscopic method. For that we present a novel
  calibration of microturbulence based on 3D model atmospheres. The
  second method is the classical spectroscopic analysis based on Fe
  lines. We also tested two different line lists in an attempt to
  minimize possible non-LTE effects and to optimize the treatment of
  the giants. <BR /> Results: We show that it is possible to obtain a
  consistent metallicity scale between dwarfs and giants. The preferred
  method should constrain the three parameters T<SUB>eff</SUB>, log g,
  and ξ independent of spectroscopy. A careful selection of Fe lines is
  also important. In particular, the lines should not be chosen based
  on the Sun or other dwarfs, but specifically to be free of blends in
  the spectra of giants. When attention is paid to the line list, the
  classical spectroscopic method can also produce consistent results. In
  our test, the metallicities derived with the well-constrained set
  of stellar parameters are consistent independent of the line list
  used. Therefore, for this cluster we favor the metallicity of +0.18
  ± 0.03 dex obtained with this method. The classical spectroscopic
  analysis, using the line list optimized for the giants, provides a
  metallicity of +0.14 ± 0.03 dex, in agreement with previous works. <P
  />Based on data obtained from the ESO Science Archive Facility. The
  observations were made with ESO Telescopes at the La Silla and Paranal
  Observatories under programmes ID 070.D-0356, 088.C-0513 and 070.D-0421.

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

---------------------------------------------------------
Title: Chemical composition of a sample of bright solar-metallicity
    stars
Authors: Caffau, E.; Mott, A.; Steffen, M.; Bonifacio, P.; Strassmeier,
   K. G.; Gallagher, A.; Faraggiana, R.; Sbordone, L.
2015AN....336..968C    Altcode: 2015arXiv151004269C
  We present a detailed analysis of seven young stars observed with the
  spectrograph SOPHIE at the Observatoire de Haute-Provence for which the
  chemical composition was incomplete or absent in the literature. For
  five stars, we derived the stellar parameters and chemical compositions
  using our automatic pipeline optimized for F, G, and K stars, while
  for the other two stars with high rotational velocity, we derived the
  stellar parameters by using other information (parallax), and performed
  a line-by-line analysis. Chromospheric emission-line fluxes from Ca
  II are obtained for all targets. The stellar parameters we derive are
  generally in good agreement with what is available in the literature. We
  provide a chemical analysis of two of the stars for the first time. The
  star HIP 80124 shows a strong Li feature at 670.8 nm implying a high
  lithium abundance. Its chemical pattern is not consistent with it
  being a solar sibling, as has been suggested. <P />Data obtained at
  Observatoire de Haute Provence, with the SOPHIE spectrograph.

---------------------------------------------------------
Title: The photospheric solar oxygen project. IV. 3D-NLTE
    investigation of the 777 nm triplet lines
Authors: Steffen, M.; Prakapavičius, D.; Caffau, E.; Ludwig, H. -G.;
   Bonifacio, P.; Cayrel, R.; Kučinskas, A.; Livingston, W. C.
2015A&A...583A..57S    Altcode: 2015arXiv150803487S
  Context. The solar photospheric oxygen abundance is still widely
  debated. Adopting the solar chemical composition based on the "low"
  oxygen abundance, as determined with the use of three-dimensional (3D)
  hydrodynamical model atmospheres, results in a well-known mismatch
  between theoretical solar models and helioseismic measurements
  that is so far unresolved. <BR /> Aims: We carry out an independent
  redetermination of the solar oxygen abundance by investigating the
  center-to-limb variation of the O i IR triplet lines at 777 nm in
  different sets of spectra. <BR /> Methods: The high-resolution and high
  signal-to-noise solar center-to-limb spectra are analyzed with the
  help of detailed synthetic line profiles based on 3D hydrodynamical
  CO5BOLD model atmospheres and 3D non-LTE line formation calculations
  with NLTE3D. The idea is to exploit the information contained in the
  observations at different limb angles to simultaneously derive the
  oxygen abundance, A(O), and the scaling factor S<SUB>H</SUB> that
  describes the cross-sections for inelastic collisions with neutral
  hydrogen relative to the classical Drawin formula. Using the same
  codes and methods, we compare our 3D results with those obtained from
  the semi-empirical Holweger-Müller model atmosphere as well as from
  different one-dimensional (1D) reference models. <BR /> Results: With
  the CO5BOLD 3D solar model, the best fit of the center-to-limb variation
  of the triplet lines is obtained when the collisions by neutral hydrogen
  atoms are assumed to be efficient, i.e., when the scaling factor
  S<SUB>H</SUB> is between 1.2 and 1.8, depending on the choice of the
  observed spectrum and the triplet component used in the analysis. The
  line profile fits achieved with standard 1D model atmospheres (with
  fixed microturbulence, independent of disk position μ) are clearly
  of inferior quality compared to the 3D case, and give the best match
  to the observations when ignoring collisions with neutral hydrogen
  (S<SUB>H</SUB> = 0). The results derived with the Holweger-Müller model
  are intermediate between 3D and standard 1D. <BR /> Conclusions: The
  analysis of various observations of the triplet lines with different
  methods yields oxygen abundance values (on a logarithmic scale where
  A(H) = 12) that fall in the range 8.74 &lt;A(O) &lt; 8.78, and our
  best estimate of the 3D non-LTE solar oxygen abundance is A(O) = 8.76
  ± 0.02. All 1D non-LTE models give much lower oxygen abundances,
  by up to -0.15 dex. This is mainly a consequence of the assumption
  of a μ-independent microturbulence. An independent determination of
  the relevant collisional cross-sections is essential to substantially
  improve the accuracy of the oxygen abundance derived from the O i IR
  triplet. <P />Appendices E and F are available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201526406/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: On the Evolution of Magnetic White Dwarfs
Authors: Tremblay, P. -E.; Fontaine, G.; Freytag, B.; Steiner, O.;
   Ludwig, H. -G.; Steffen, M.; Wedemeyer, S.; Brassard, P.
2015ApJ...812...19T    Altcode: 2015arXiv150905398T
  We present the first radiation magnetohydrodynamic simulations of the
  atmosphere of white dwarf stars. We demonstrate that convective energy
  transfer is seriously impeded by magnetic fields when the plasma-β
  parameter, the thermal-to-magnetic-pressure ratio, becomes smaller
  than unity. The critical field strength that inhibits convection
  in the photosphere of white dwarfs is in the range B = 1-50 kG,
  which is much smaller than the typical 1-1000 MG field strengths
  observed in magnetic white dwarfs, implying that these objects have
  radiative atmospheres. We have employed evolutionary models to study the
  cooling process of high-field magnetic white dwarfs, where convection
  is entirely suppressed during the full evolution (B ≳ 10 MG). We
  find that the inhibition of convection has no effect on cooling rates
  until the effective temperature (T<SUB>eff</SUB>) reaches a value of
  around 5500 K. In this regime, the standard convective sequences start
  to deviate from the ones without convection due to the convective
  coupling between the outer layers and the degenerate reservoir of
  thermal energy. Since no magnetic white dwarfs are currently known
  at the low temperatures where this coupling significantly changes the
  evolution, the effects of magnetism on cooling rates are not expected
  to be observed. This result contrasts with a recent suggestion
  that magnetic white dwarfs with T<SUB>eff</SUB> ≲ 10,000 K cool
  significantly slower than non-magnetic degenerates.

---------------------------------------------------------
Title: 3D Model Atmospheres for Extremely Low-mass White Dwarfs
Authors: Tremblay, P. -E.; Gianninas, A.; Kilic, M.; Ludwig, H. -G.;
   Steffen, M.; Freytag, B.; Hermes, J. J.
2015ApJ...809..148T    Altcode: 2015arXiv150701927T
  We present an extended grid of mean three-dimensional (3D) spectra
  for low-mass, pure-hydrogen atmosphere DA white dwarfs (WDs). We use
  CO5BOLD radiation-hydrodynamics 3D simulations covering T<SUB>eff</SUB>
  = 6000-11,500 K and log g = 5-6.5 (g in cm s<SUP>-2</SUP>) to derive
  analytical functions to convert spectroscopically determined 1D
  temperatures and surface gravities to 3D atmospheric parameters. Along
  with the previously published 3D models, the 1D to 3D corrections are
  now available for essentially all known convective DA WDs (i.e., log g
  = 5-9). For low-mass WDs, the correction in temperature is relatively
  small (a few percent at the most), but the surface gravities measured
  from the 3D models are lower by as much as 0.35 dex. We revisit
  the spectroscopic analysis of the extremely low-mass (ELM) WDs, and
  demonstrate that the 3D models largely resolve the discrepancies seen
  in the radius and mass measurements for relatively cool ELM WDs in
  eclipsing double WD and WD + millisecond pulsar binary systems. We
  also use the 3D corrections to revise the boundaries of the ZZ Ceti
  instability strip, including the recently found ELM pulsators.

---------------------------------------------------------
Title: The photospheric solar oxygen project. III. Investigation of
    the centre-to-limb variation of the 630 nm [O I]-Ni I blend
Authors: Caffau, E.; Ludwig, H. -G.; Steffen, M.; Livingston, W.;
   Bonifacio, P.; Malherbe, J. -M.; Doerr, H. -P.; Schmidt, W.
2015A&A...579A..88C    Altcode: 2015arXiv150600931C
  Context. The solar photospheric abundance of oxygen is still a matter
  of debate. For about ten years some determinations have favoured a
  low oxygen abundance which is at variance with the value inferred by
  helioseismology. Among the oxygen abundance indicators, the forbidden
  line at 630 nm has often been considered the most reliable even
  though it is blended with a Ni i line. In Papers I and II of this
  series we reported a discrepancy in the oxygen abundance derived
  from the 630 nm and the subordinate [O I] line at 636 nm in dwarf
  stars, including the Sun. <BR /> Aims: Here we analyse several,
  in part new, solar observations of the centre-to-limb variation
  of the spectral region including the blend at 630 nm in order to
  separate the individual contributions of oxygen and nickel. <BR />
  Methods: We analyse intensity spectra observed at different limb
  angles in comparison with line formation computations performed on a
  CO5BOLD 3D hydrodynamical simulation of the solar atmosphere. <BR />
  Results: The oxygen abundances obtained from the forbidden line at
  different limb angles are inconsistent if the commonly adopted nickel
  abundance of 6.25 is assumed in our local thermodynamic equilibrium
  computations. With a slightly lower nickel abundance, A(Ni) ≈ 6.1,
  we obtain consistent fits indicating an oxygen abundance of A(O) = 8.73
  ± 0.05. At this value the discrepancy with the subordinate oxygen
  line remains. <BR /> Conclusions: The derived value of the oxygen
  abundance supports the notion of a rather low oxygen abundance in the
  solar photosphere. However, it is disconcerting that the forbidden
  oxygen lines at 630 and 636 nm give noticeably different results,
  and that the nickel abundance derived here from the 630 nm blend is
  lower than expected from other nickel lines.

---------------------------------------------------------
Title: TOPoS . II. On the bimodality of carbon abundance in CEMP
    stars Implications on the early chemical evolution of galaxies
Authors: Bonifacio, P.; Caffau, E.; Spite, M.; Limongi, M.; Chieffi,
   A.; Klessen, R. S.; François, P.; Molaro, P.; Ludwig, H. -G.; Zaggia,
   S.; Spite, F.; Plez, B.; Cayrel, R.; Christlieb, N.; Clark, P. C.;
   Glover, S. C. O.; Hammer, F.; Koch, A.; Monaco, L.; Sbordone, L.;
   Steffen, M.
2015A&A...579A..28B    Altcode: 2015arXiv150405963B
  Context. In the course of the Turn Off Primordial Stars (TOPoS) survey,
  aimed at discovering the lowest metallicity stars, we have found several
  carbon-enhanced metal-poor (CEMP) stars. These stars are very common
  among the stars of extremely low metallicity and provide important
  clues to the star formation processes. We here present our analysis
  of six CEMP stars. <BR /> Aims: We want to provide the most complete
  chemical inventory for these six stars in order to constrain the
  nucleosynthesis processes responsible for the abundance patterns. <BR
  /> Methods: We analyse both X-Shooter and UVES spectra acquired at the
  VLT. We used a traditional abundance analysis based on OSMARCS 1D local
  thermodynamic equilibrium (LTE) model atmospheres and the turbospectrum
  line formation code. <BR /> Results: Calcium and carbon are the only
  elements that can be measured in all six stars. The range is -5.0 ≤
  [Ca/H] &lt;-2.1 and 7.12 ≤ A(C) ≤ 8.65. For star SDSS J1742+2531
  we were able to detect three Fe i lines from which we deduced [Fe/H]
  = -4.80, from four Ca ii lines we derived [Ca/H] = -4.56, and from
  synthesis of the G-band we derived A(C) = 7.26. For SDSS J1035+0641 we
  were not able to detect any iron lines, yet we could place a robust
  (3σ) upper limit of [Fe/H] &lt; -5.0 and measure the Ca abundance,
  with [Ca/H] = -5.0, and carbon, A(C) = 6.90, suggesting that this star
  could be even more metal-poor than SDSS J1742+2531. This makes these
  two stars the seventh and eighth stars known so far with [Fe/H] &lt;
  -4.5, usually termed ultra-iron-poor (UIP) stars. No lithium is detected
  in the spectrum of SDSS J1742+2531 or SDSS J1035+0641, which implies a
  robust upper limit of A(Li) &lt; 1.8 for both stars. <BR /> Conclusions:
  Our measured carbon abundances confirm the bimodal distribution of
  carbon in CEMP stars, identifying a high-carbon band and a low-carbon
  band. We propose an interpretation of this bimodality according to which
  the stars on the high-carbon band are the result of mass transfer from
  an AGB companion, while the stars on the low-carbon band are genuine
  fossil records of a gas cloud that has also been enriched by a faint
  supernova (SN) providing carbon and the lighter elements. The abundance
  pattern of the UIP stars shows a large star-to-star scatter in the
  [X/Ca] ratios for all elements up to aluminium (up to 1 dex), but
  this scatter drops for heavier elements and is at most of the order
  of a factor of two. We propose that this can be explained if these
  stars are formed from gas that has been chemically enriched by several
  SNe, that produce the roughly constant [X/Ca] ratios for the heavier
  elements, and in some cases the gas has also been polluted by the
  ejecta of a faint SN that contributes the lighter elements in variable
  amounts. The absence of lithium in four of the five known unevolved
  UIP stars can be explained by a dominant role of fragmentation in the
  formation of these stars. This would result either in a destruction
  of lithium in the pre-main-sequence phase, through rotational mixing
  or to a lack of late accretion from a reservoir of fresh gas. The
  phenomenon should have varying degrees of efficiency. <P />Based on
  observations obtained at ESO Paranal Observatory, programme 091.D-0288,
  091.D-0305, 189.D-0165.Appendix A is available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201425266/olm">http://www.aanda.org</A>Tables
  4 is only available at the CDS via anonymous ftp to <A
  href="http://cdsarc.u-strasbg.fr">http://cdsarc.u-strasbg.fr</A>
  (ftp://130.79.128.5) or via <A
  href="http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/579/A28">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/579/A28</A>

---------------------------------------------------------
Title: Calibration of the Mixing-Length Free Parameter for White
    Dwarf Structures
Authors: Tremblay, P. -E.; Ludwig, H. -G.; Freytag, B.; Fontaine,
   G.; Steffen, M.; Brassard, P.
2015ASPC..493...89T    Altcode:
  We present a comparison of our grid of 3D radiation-hydrodynamical
  simulations for 70 pure-hydrogen DA white dwarfs, in the surface
  gravity range 7.0 ≤log g≤ 9.0, with 1D envelope models based on the
  mixing-length theory (MLT) for convection. We perform a calibration
  of the mixing-length parameter for the lower part of the convection
  zone. The 3D simulations are often restricted to the upper convective
  layers, and in those cases, we rely on the asymptotic entropy value of
  the adiabatic 3D upflows to calibrate 1D envelopes. Our results can be
  applied to 1D structure calculations, and in particular for pulsation
  and convective mixing studies. We demonstrate that while the 1D MLT
  only provides a bottom boundary of the convection zone based on the
  Schwarzschild criterion, the 3D stratifications are more complex. There
  is a large overshoot region below the convective layers that is likely
  critical for chemical diffusion applications.

---------------------------------------------------------
Title: The Born-again Planetary Nebulae Abell 30 and Abell 78
Authors: Todt, H.; Guerrero, M. A.; Fang, X.; Toala, J. A.;
   Arthur, J. S.; Blair, W. P.; Chu, Y. -H.; Gruendl, R. A.; Hamann,
   W. -R.; Marquez-Lugo, R. A.; Oskinova, L.; Ruiz, N.; Steffen, M.;
   Schoenberner, D.
2015ASPC..493..141T    Altcode:
  The planetary nebulae Abell 30 and Abell 78 are born-again nebulae,
  which are believed to have undergone a very late thermal pulse,
  resulting in the ejection of hydrogen-poor material. Born-again PNe
  are a rare phenomenon, only a few are known. It is really intriguing
  that in all cases the expansion of the hydrogen-poor ejecta is highly
  asymmetrical. Here we present new HST observations of the expansion
  of the ejecta in Abell 30 and Abell 78, and compare them to ≍20 yrs
  older HST images.

---------------------------------------------------------
Title: VizieR Online Data Catalog: Abundances of 3 CEMP stars
    (Bonifacio+, 2015)
Authors: Bonifacio, P.; Caffau, E.; Spite, M.; Limongi, M.; Chieffi,
   A.; Klessen, R. S.; Francois, P.; Molaro, P.; Ludwig, H. -G.; Zaggia,
   S.; Spite, F.; Plez, B.; Cayrel, R.; Christlieb, N.; Clark, P. C.;
   Glover, S. C. O.; Hammer, F.; Koch, A.; Monaco, L.; Sbordone, L.;
   Steffen, M.
2015yCat..35790028B    Altcode:
  We analyse both X-Shooter and UVES spectra acquired at the VLT. We used
  a traditional abundance analysis based on OSMARCS 1D Local Thermodynamic
  Equilibrium (LTE) model atmospheres and the TURBOSPECTRUM line formation
  code. <P />(2 data files).

---------------------------------------------------------
Title: Three-dimensional hydrodynamical CO<SUP>5</SUP>BOLD model
    atmospheres of red giant stars. IV. Oxygen diagnostics in extremely
    metal-poor red giants with infrared OH lines
Authors: Dobrovolskas, V.; Kučinskas, A.; Bonifacio, P.; Caffau,
   E.; Ludwig, H. -G.; Steffen, M.; Spite, M.
2015A&A...576A.128D    Altcode: 2015arXiv150206587D
  Context. Although oxygen is an important tracer of Galactic chemical
  evolution, measurements of its abundance in the atmospheres of the
  oldest Galactic stars are still scarce and rather imprecise. This
  is mainly because only a few spectral lines are available for the
  abundance diagnostics. At the lowest end of the metallicity scale,
  oxygen can only be measured in giant stars and in most of cases such
  measurements rely on a single forbidden [O i] 630 nm line that is very
  weak and frequently blended with telluric lines. Although molecular
  OH lines located in the ultraviolet and infrared could also be used
  for the diagnostics, oxygen abundances obtained from the OH lines and
  the [O i] 630 nm line are usually discrepant to a level of ~ 0.3-0.4
  dex. <BR /> Aims: We study the influence of convection on the formation
  of the infrared (IR) OH lines and the forbidden [O i] 630 nm line in the
  atmospheres of extremely metal-poor (EMP) red giant stars. Our ultimate
  goal is to clarify whether a realistic treatment of convection with
  state-of-the-art 3D hydrodynamical model atmospheres may help to bring
  the oxygen abundances obtained using the two indicators into closer
  agreement. <BR /> Methods: We used high-resolution (R = 50 000) and high
  signal-to-noise ratio (S/N ≈ 200-600) spectra of four EMP red giant
  stars obtained with the VLT CRIRES spectrograph. For each EMP star,
  4-14 IR OH vibrational-rotational lines located in the spectral range of
  1514-1548 and 1595-1632 nm were used to determine oxygen abundances by
  employing standard 1D local thermodynamic equilibrium (LTE) abundance
  analysis methodology. We then corrected the 1D LTE abundances
  obtained from each individual OH line for the 3D hydrodynamical
  effects, which was done by applying 3D-1D LTE abundance corrections
  that were determined using 3D hydrodynamical CO<SUP>5</SUP>BOLD and
  1D hydrostatic LHD model atmospheres. <BR /> Results: We find that
  the influence of convection on the formation of [O i] 630 nm line in
  the atmospheres of EMP giants studied here is minor, which leads to
  very small 3D-1D abundance corrections (Δ<SUB>3D-1D</SUB> ≤ -0.01
  dex). On the contrary, IR OH lines are strongly affected by convection
  and thus the abundance corrections for these lines are significant,
  Δ<SUB>3D-1D</SUB> ≈ -0.2···-0.3 dex. These abundance corrections
  do indeed bring the 1D LTE oxygen abundances of EMP red giants obtained
  using IR OH lines into better agreement with those determined from the
  [O i] 630 nm line. Since in the EMP red giants IR OH lines are typically
  at least a factor of two stronger than the [O i] line, OH lines may be
  useful indicators of oxygen abundances in the EMP stars, provided that
  the analysis is based on 3D hydrodynamical model atmospheres. <P />Based
  on observations obtained at the European Southern Observatory (ESO)
  Very Large Telescope (VLT) at Paranal Observatory, Chile (observing
  programme 089.D-0079).Appendices are available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201424885/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: The Chandra Planetary Nebula Survey (ChanPlaNS). III. X-Ray
    Emission from the Central Stars of Planetary Nebulae
Authors: Montez, R., Jr.; Kastner, J. H.; Balick, B.; Behar, E.;
   Blackman, E.; Bujarrabal, V.; Chu, Y. -H.; Corradi, R. L. M.; De Marco,
   O.; Frank, A.; Freeman, M.; Frew, D. J.; Guerrero, M. A.; Jones, D.;
   Lopez, J. A.; Miszalski, B.; Nordhaus, J.; Parker, Q. A.; Sahai, R.;
   Sandin, C.; Schonberner, D.; Soker, N.; Sokoloski, J. L.; Steffen,
   M.; Toalá, J. A.; Ueta, T.; Villaver, E.; Zijlstra, A.
2015ApJ...800....8M    Altcode: 2014arXiv1412.2793M
  We present X-ray spectral analysis of 20 point-like X-ray sources
  detected in Chandra Planetary Nebula Survey observations of 59 planetary
  nebulae (PNe) in the solar neighborhood. Most of these 20 detections
  are associated with luminous central stars within relatively young,
  compact nebulae. The vast majority of these point-like X-ray-emitting
  sources at PN cores display relatively "hard" (&gt;=0.5 keV) X-ray
  emission components that are unlikely to be due to photospheric emission
  from the hot central stars (CSPN). Instead, we demonstrate that these
  sources are well modeled by optically thin thermal plasmas. From the
  plasma properties, we identify two classes of CSPN X-ray emission:
  (1) high-temperature plasmas with X-ray luminosities, L <SUB>X</SUB>,
  that appear uncorrelated with the CSPN bolometric luminosity, L
  <SUB>bol</SUB> and (2) lower-temperature plasmas with L <SUB>X</SUB>/L
  <SUB>bol</SUB> ~ 10<SUP>-7</SUP>. We suggest these two classes
  correspond to the physical processes of magnetically active binary
  companions and self-shocking stellar winds, respectively. In many cases
  this conclusion is supported by corroborative multiwavelength evidence
  for the wind and binary properties of the PN central stars. By thus
  honing in on the origins of X-ray emission from PN central stars,
  we enhance the ability of CSPN X-ray sources to constrain models of
  PN shaping that invoke wind interactions and binarity.

---------------------------------------------------------
Title: Calibration of the Mixing-length Theory for Convective White
    Dwarf Envelopes
Authors: Tremblay, P. -E.; Ludwig, H. -G.; Freytag, B.; Fontaine,
   G.; Steffen, M.; Brassard, P.
2015ApJ...799..142T    Altcode: 2014arXiv1412.1789T
  A calibration of the mixing-length parameter in the local mixing-length
  theory (MLT) is presented for the lower part of the convection zone in
  pure-hydrogen-atmosphere white dwarfs. The parameterization is performed
  from a comparison of three-dimensional (3D) CO5BOLD simulations with
  a grid of one-dimensional (1D) envelopes with a varying mixing-length
  parameter. In many instances, the 3D simulations are restricted to the
  upper part of the convection zone. The hydrodynamical calculations
  suggest, in those cases, that the entropy of the upflows does not
  change significantly from the bottom of the convection zone to regions
  immediately below the photosphere. We rely on this asymptotic entropy
  value, characteristic of the deep and adiabatically stratified layers,
  to calibrate 1D envelopes. The calibration encompasses the convective
  hydrogen-line (DA) white dwarfs in the effective temperature range
  6000 &lt;= T <SUB>eff</SUB> (K) &lt;=15, 000 and the surface gravity
  range 7.0 &lt;= log g &lt;= 9.0. It is established that the local
  MLT is unable to reproduce simultaneously the thermodynamical, flux,
  and dynamical properties of the 3D simulations. We therefore propose
  three different parameterizations for these quantities. The resulting
  calibration can be applied to structure and envelope calculations,
  in particular for pulsation, chemical diffusion, and convective mixing
  studies. On the other hand, convection has no effect on the white dwarf
  cooling rates until there is a convective coupling with the degenerate
  core below T <SUB>eff</SUB> ~ 5000 K. In this regime, the 1D structures
  are insensitive to the MLT parameterization and converge to the mean
  3D results, hence they remain fully appropriate for age determinations.

---------------------------------------------------------
Title: Oxygen in the Early Galaxy: OH Lines as Tracers of Oxygen
    Abundance in Extremely Metal-Poor Giant Stars
Authors: Kucinskas, A.; Dobrovolskas, V.; Bonifacio, P.; Caffau, E.;
   Ludwig, H. -G.; Steffen, M.; Spite, M.
2015csss...18..327K    Altcode: 2014arXiv1409.3153K
  Oxygen is a powerful tracer element of Galactic chemical
  evolution. Unfortunately, only a few oxygen lines are available in the
  ultraviolet-infrared stellar spectra for the reliable determination of
  its abundance. Moreover, oxygen abundances obtained using different
  spectral lines often disagree significantly. In this contribution we
  therefore investigate whether the inadequate treatment of convection in
  1D hydrostatic model atmospheres used in the abundance determinations
  may be responsible for this disagreement. For this purpose, we used VLT
  CRIRES spectra of three EMP giants, as well as 3D hydrodynamical COBOLD
  and 1D hydrostatic LHD model atmospheres, to investigate the role of
  convection in the formation of infrared (IR) OH lines. Our results show
  that the presence of convection leads to significantly stronger IR OH
  lines. As a result, the difference in the oxygen abundance determined
  from IR OH lines with 3D hydrodynamical and classical 1D hydrostatic
  model atmospheres may reach -0.2 dots -0.3 dex. In case of the three
  EMP giants studied here, we obtain a good agrement between the 3D LTE
  oxygen abundances determined by us using vibrational-rotational IR
  OH lines in the spectral range of 1514-1626 nm, and oxygen abundances
  determined from forbidden [O I] 630 nm line in previous studies.

---------------------------------------------------------
Title: Properties of small-scale magnetism of stellar atmospheres
Authors: Steiner, Oskar; Salhab, René; Freytag, Bernd; Rajaguru,
   Paul; Schaffenberger, Werner; Steffen, Matthias
2014PASJ...66S...5S    Altcode: 2014PASJ..tmp...95S
  The magnetic field outside of sunspots is concentrated in the
  intergranular space, where it forms a delicate filigree of bright
  ribbons and dots as seen on broad band images of the Sun. We expect this
  small-scale magnetic field to exhibit a similar behavior in stellar
  atmospheres. In order to find out more about it, we perform numerical
  simulations of the surface layers of stellar atmospheres. Here, we
  report on preliminary results from simulations in the range between
  4000 K and 6500 K effective temperature with an initial vertical,
  homogeneous magnetic field of 50 G strength. We find that the field
  strength of the strongest magnetic flux concentrations increases with
  decreasing effective temperature at the height level where the average
  Rosseland optical depth is one. On the other hand, at the same level,
  the field is less strong than the thermal equipartition value in the
  coolest model but assumes superequipartition in the models hotter
  than 5000 K. While the Wilson depression of the strongest field
  concentrations is about one pressure scale height in the coolest
  model, it is more than four times the pressure scale height in the
  hottest one. We also find that the relative contribution of the bright
  filigree to the bolometric, vertically directed radiative intensity is
  most significant for the T<SUB>eff</SUB> = 5000 K model (0.6%-0.79%)
  and least significant for the hottest and coolest models (0.1%-0.46%
  and 0.14%-0.32%, respectively). This behavior suggests that the effect
  of the small-scale magnetic field on the photometric variability is more
  significant for K dwarf stars than for F-type and also M-type stars.

---------------------------------------------------------
Title: Detecting weak magnetic fields in the central stars of
    planetary nebulae
Authors: Steffen, M.; Hubrig, S.; Todt, H.; Schöller, M.; Sandin,
   C.; Hamann, W. -R.; Schönberner, D.
2014psce.conf..351S    Altcode:
  We have carried out low-resolution spectropolarimetric observations
  with FORS 2, installed on the VLT, ESO, of a representative sample
  of 12 bright central stars of Planetary Nebulae (PNe) with different
  morphology. Two of the sample are hydrogen-deficient (Wolf-Rayet
  type) stars. Our measurements rule out the existence of strong global
  magnetic fields of the order of kG in any of the PN central stars of
  our sample. Even so, our data may indicate the presence of weak mean
  longitudinal magnetic fields of a few hundred Gauss in the central
  stars of two elliptical nebulae, IC 418 and NGC 2392, and a very weak
  magnetic field of about 100 G in the Wolf-Rayet type central star
  Hen 2-113. However, the significance of these marginal detections
  depends on the method adopted for estimating the uncertainties in the
  magnetic-field measurements.

---------------------------------------------------------
Title: The Chandra Planetary Nebula Survey (ChanPlaNS). II. X-Ray
    Emission from Compact Planetary Nebulae
Authors: Freeman, M.; Montez, R., Jr.; Kastner, J. H.; Balick, B.;
   Frew, D. J.; Jones, D.; Miszalski, B.; Sahai, R.; Blackman, E.;
   Chu, Y. -H.; De Marco, O.; Frank, A.; Guerrero, M. A.; Lopez, J. A.;
   Zijlstra, A.; Bujarrabal, V.; Corradi, R. L. M.; Nordhaus, J.; Parker,
   Q. A.; Sandin, C.; Schönberner, D.; Soker, N.; Sokoloski, J. L.;
   Steffen, M.; Toalá, J. A.; Ueta, T.; Villaver, E.
2014ApJ...794...99F    Altcode: 2014arXiv1407.4141F
  We present results from the most recent set of observations obtained
  as part of the Chandra X-ray observatory Planetary Nebula Survey
  (ChanPlaNS), the first comprehensive X-ray survey of planetary nebulae
  (PNe) in the solar neighborhood (i.e., within ~1.5 kpc of the Sun). The
  survey is designed to place constraints on the frequency of appearance
  and range of X-ray spectral characteristics of X-ray-emitting PN
  central stars and the evolutionary timescales of wind-shock-heated
  bubbles within PNe. ChanPlaNS began with a combined Cycle 12 and
  archive Chandra survey of 35 PNe. ChanPlaNS continued via a Chandra
  Cycle 14 Large Program which targeted all (24) remaining known
  compact (R <SUB>neb</SUB> &lt;~ 0.4 pc), young PNe that lie within
  ~1.5 kpc. Results from these Cycle 14 observations include first-time
  X-ray detections of hot bubbles within NGC 1501, 3918, 6153, and 6369,
  and point sources in HbDs 1, NGC 6337, and Sp 1. The addition of the
  Cycle 14 results brings the overall ChanPlaNS diffuse X-ray detection
  rate to ~27% and the point source detection rate to ~36%. It has
  become clearer that diffuse X-ray emission is associated with young
  (lsim 5 × 10<SUP>3</SUP> yr), and likewise compact (R <SUB>neb</SUB>
  &lt;~ 0.15 pc), PNe with closed structures and high central electron
  densities (n<SUB>e</SUB> &gt;~ 1000 cm<SUP>-3</SUP>), and is rarely
  associated with PNe that show H<SUB>2</SUB> emission and/or pronounced
  butterfly structures. Hb 5 is one such exception of a PN with a
  butterfly structure that hosts diffuse X-ray emission. Additionally,
  two of the five new diffuse X-ray detections (NGC 1501 and NGC 6369)
  host [WR]-type central stars, supporting the hypothesis that PNe with
  central stars of [WR]-type are likely to display diffuse X-ray emission.

---------------------------------------------------------
Title: The Gaia-ESO Survey: The analysis of high-resolution UVES
    spectra of FGK-type stars
Authors: Smiljanic, R.; Korn, A. J.; Bergemann, M.; Frasca, A.;
   Magrini, L.; Masseron, T.; Pancino, E.; Ruchti, G.; San Roman,
   I.; Sbordone, L.; Sousa, S. G.; Tabernero, H.; Tautvaišienė,
   G.; Valentini, M.; Weber, M.; Worley, C. C.; Adibekyan, V. Zh.;
   Allende Prieto, C.; Barisevičius, G.; Biazzo, K.; Blanco-Cuaresma,
   S.; Bonifacio, P.; Bragaglia, A.; Caffau, E.; Cantat-Gaudin, T.;
   Chorniy, Y.; de Laverny, P.; Delgado-Mena, E.; Donati, P.; Duffau,
   S.; Franciosini, E.; Friel, E.; Geisler, D.; González Hernández,
   J. I.; Gruyters, P.; Guiglion, G.; Hansen, C. J.; Heiter, U.; Hill, V.;
   Jacobson, H. R.; Jofre, P.; Jönsson, H.; Lanzafame, A. C.; Lardo, C.;
   Ludwig, H. -G.; Maiorca, E.; Mikolaitis, Š.; Montes, D.; Morel, T.;
   Mucciarelli, A.; Muñoz, C.; Nordlander, T.; Pasquini, L.; Puzeras,
   E.; Recio-Blanco, A.; Ryde, N.; Sacco, G.; Santos, N. C.; Serenelli,
   A. M.; Sordo, R.; Soubiran, C.; Spina, L.; Steffen, M.; Vallenari,
   A.; Van Eck, S.; Villanova, S.; Gilmore, G.; Randich, S.; Asplund,
   M.; Binney, J.; Drew, J.; Feltzing, S.; Ferguson, A.; Jeffries, R.;
   Micela, G.; Negueruela, I.; Prusti, T.; Rix, H. -W.; Alfaro, E.;
   Babusiaux, C.; Bensby, T.; Blomme, R.; Flaccomio, E.; François, P.;
   Irwin, M.; Koposov, S.; Walton, N.; Bayo, A.; Carraro, G.; Costado,
   M. T.; Damiani, F.; Edvardsson, B.; Hourihane, A.; Jackson, R.; Lewis,
   J.; Lind, K.; Marconi, G.; Martayan, C.; Monaco, L.; Morbidelli, L.;
   Prisinzano, L.; Zaggia, S.
2014A&A...570A.122S    Altcode: 2014arXiv1409.0568S
  Context. The ongoing Gaia-ESO Public Spectroscopic Survey is using
  FLAMES at the VLT to obtain high-quality medium-resolution Giraffe
  spectra for about 10<SUP>5</SUP> stars and high-resolution UVES spectra
  for about 5000 stars. With UVES, the Survey has already observed
  1447 FGK-type stars. <BR /> Aims: These UVES spectra are analyzed
  in parallel by several state-of-the-art methodologies. Our aim is
  to present how these analyses were implemented, to discuss their
  results, and to describe how a final recommended parameter scale is
  defined. We also discuss the precision (method-to-method dispersion)
  and accuracy (biases with respect to the reference values) of the
  final parameters. These results are part of the Gaia-ESO second
  internal release and will be part of its first public release of
  advanced data products. <BR /> Methods: The final parameter scale is
  tied to the scale defined by the Gaia benchmark stars, a set of stars
  with fundamental atmospheric parameters. In addition, a set of open
  and globular clusters is used to evaluate the physical soundness
  of the results. Each of the implemented methodologies is judged
  against the benchmark stars to define weights in three different
  regions of the parameter space. The final recommended results are
  the weighted medians of those from the individual methods. <BR />
  Results: The recommended results successfully reproduce the atmospheric
  parameters of the benchmark stars and the expected T<SUB>eff</SUB>-log
  g relation of the calibrating clusters. Atmospheric parameters and
  abundances have been determined for 1301 FGK-type stars observed with
  UVES. The median of the method-to-method dispersion of the atmospheric
  parameters is 55 K for T<SUB>eff</SUB>, 0.13 dex for log g and 0.07
  dex for [Fe/H]. Systematic biases are estimated to be between 50-100
  K for T<SUB>eff</SUB>, 0.10-0.25 dex for log g and 0.05-0.10 dex for
  [Fe/H]. Abundances for 24 elements were derived: C, N, O, Na, Mg, Al,
  Si, Ca, Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Y, Zr, Mo, Ba, Nd, and
  Eu. The typical method-to-method dispersion of the abundances varies
  between 0.10 and 0.20 dex. <BR /> Conclusions: The Gaia-ESO sample of
  high-resolution spectra of FGK-type stars will be among the largest of
  its kind analyzed in a homogeneous way. The extensive list of elemental
  abundances derived in these stars will enable significant advances in
  the areas of stellar evolution and Milky Way formation and evolution. <P
  />Based on observations made with the ESO/VLT, at Paranal Observatory,
  under program 188.B-3002 (The Gaia-ESO Public Spectroscopic Survey, PIs
  Gilmore and Randich). Appendices are available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201423937/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: Weak magnetic fields in central stars of planetary nebulae?
Authors: Steffen, M.; Hubrig, S.; Todt, H.; Schöller, M.; Hamann,
   W. -R.; Sandin, C.; Schönberner, D.
2014A&A...570A..88S    Altcode: 2014arXiv1408.3000S
  Context. It is not yet clear whether magnetic fields play an essential
  role in shaping planetary nebulae (PNe), or whether stellar rotation
  alone and/or a close binary companion, stellar or substellar, can
  account for the variety of the observed nebular morphologies. <BR />
  Aims: In a quest for empirical evidence verifying or disproving the
  role of magnetic fields in shaping planetary nebulae, we follow up on
  previous attempts to measure the magnetic field in a representative
  sample of PN central stars. <BR /> Methods: We obtained low-resolution
  polarimetric spectra with FORS 2 installed on the Antu telescope of
  the VLT for a sample of 12 bright central stars of PNe with different
  morphologies, including two round nebulae, seven elliptical nebulae,
  and three bipolar nebulae. Two targets are Wolf-Rayet type central
  stars. <BR /> Results: For the majority of the observed central stars,
  we do not find any significant evidence for the existence of surface
  magnetic fields. However, our measurements may indicate the presence of
  weak mean longitudinal magnetic fields of the order of 100 Gauss in the
  central star of the young elliptical planetary nebula IC 418 as well
  as in the Wolf-Rayet type central star of the bipolar nebula Hen 2-113
  and the weak emission line central star of the elliptical nebula Hen
  2-131. A clear detection of a 250 G mean longitudinal field is achieved
  for the A-type companion of the central star of NGC 1514. Some of the
  central stars show a moderate night-to-night spectrum variability,
  which may be the signature of a variable stellar wind and/or rotational
  modulation due to magnetic features. <BR /> Conclusions: Since our
  analysis indicates only weak fields, if any, in a few targets of our
  sample, we conclude that strong magnetic fields of the order of kG are
  not widespread among PNe central stars. Nevertheless, simple estimates
  based on a theoretical model of magnetized wind bubbles suggest that
  even weak magnetic fields below the current detection limit of the
  order of 100 G may well be sufficient to contribute to the shaping of
  the surrounding nebulae throughout their evolution. Our current sample
  is too small to draw conclusions about a correlation between nebular
  morphology and the presence of stellar magnetic fields. <P />Based on
  observations obtained at the European Southern Observatory, Paranal,
  Chile (ESO program No. 088.D-0425(A)).

---------------------------------------------------------
Title: VizieR Online Data Catalog: Abundances of 47 Tuc turn-off stars
    (Dobrovolskas+, 2014)
Authors: Dobrovolskas, V.; Kucinskas, A.; Bonifacio, P.; Korotin,
   S. A.; Steffen, M.; Sbordone, L.; Caffau, E.; Ludwig, H. -G.; Royer,
   F.; Prakapavicius, D.
2014yCat..35650121D    Altcode: 2014yCat..35659121D
  Spectra of the TO stars in 47 Tuc investigated in this work were
  obtained with the GIRAFFE spectrograph in August-September, 2008,
  under the programme 081.D-0287(A) (PI: Shen). The same data set
  was independently analysed by D'Orazi et al. (2010ApJ...713L...1D,
  Cat. J/ApJ/713/L1). <P />(1 data file).

---------------------------------------------------------
Title: Abundances of lithium, oxygen, and sodium in the turn-off
    stars of Galactic globular cluster 47 Tucanae
Authors: Dobrovolskas, V.; Kučinskas, A.; Bonifacio, P.; Korotin,
   S. A.; Steffen, M.; Sbordone, L.; Caffau, E.; Ludwig, H. -G.; Royer,
   F.; Prakapavičius, D.
2014A&A...565A.121D    Altcode: 2013arXiv1311.1072D
  Context. The cluster 47 Tuc is among the most metal-rich Galactic
  globular clusters and its metallicity is similar to that of metal-poor
  disc stars and open clusters. Like other globular clusters, it
  displays variations in the abundances of elements lighter than Si,
  which is generally interpreted as evidence of the presence of multiple
  stellar populations. <BR /> Aims: We aim to determine abundances of
  Li, O, and Na in a sample of of 110 turn-off (TO) stars, in order
  to study the evolution of light elements in this cluster and to put
  our results in perspective with observations of other globular and
  open clusters, as well as with field stars. <BR /> Methods: We use
  medium resolution spectra obtained with the GIRAFFE spectrograph at
  the ESO 8.2 m Kueyen VLT telescope and use state of the art 1D model
  atmospheres and NLTE line transfer to determine the abundances. We
  also employ CO<SUP>5</SUP>BOLD hydrodynamical simulations to assess
  the impact of stellar granulation on the line formation and inferred
  abundances. <BR /> Results: Our results confirm the existence of
  Na-O abundance anti-correlation and hint towards a possible Li-O
  anti-correlation in the TO stars of 47 Tuc. At the same time,
  we find no convincing evidence supporting the existence of Li-Na
  correlation. The obtained 3D NLTE mean lithium abundance in a sample
  of 94 TO stars where Li lines were detected reliably, ⟨A(Li)<SUB>3D
  NLTE</SUB>⟩ = 1.78 ± 0.18 dex, appears to be significantly lower
  than what is observed in other globular clusters. At the same time,
  star-to-star spread in Li abundance is also larger than seen in other
  clusters. The highest Li abundance observed in 47 Tuc is about 0.1
  dex lower than the lowest Li abundance observed among the un-depleted
  stars of the metal-poor open cluster NGC 2243. <BR /> Conclusions: The
  correlations/anti-correlations among light element abundances confirm
  that chemical enrichment history of 47 Tuc was similar to that of other
  globular clusters, despite the higher metallicity of 47 Tuc. The lithium
  abundances in 47 Tuc, when put into context with observations in other
  clusters and field stars, suggest that stars that are more metal-rich
  than [Fe/H] ~ -1.0 experience significant lithium depletion during
  their lifetime on the main sequence, while the more metal-poor stars
  do not. Rather strikingly, our results suggest that initial lithium
  abundance with which the star was created may only depend on its age
  (the younger the star, the higher its Li content) and not on its
  metallicity. <P />Appendices are available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201322868/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: A super lithium-rich red-clump star in the open cluster
    Trumpler 5
Authors: Monaco, L.; Boffin, H. M. J.; Bonifacio, P.; Villanova, S.;
   Carraro, G.; Caffau, E.; Steffen, M.; Ahumada, J. A.; Beletsky, Y.;
   Beccari, G.
2014A&A...564L...6M    Altcode: 2014arXiv1403.6461M
  Context. The existence of lithium-rich low-mass red giant stars still
  represents a challenge for stellar evolution models. Stellar clusters
  are privileged environments for this kind of investigation. <BR />
  Aims: To investigate the chemical abundance pattern of the old open
  cluster Trumpler 5, we observed a sample of four red-clump stars with
  high-resolution optical spectrographs. One of them (#3416) reveals
  extremely strong lithium lines in its spectrum. <BR /> Methods:
  One-dimensional, local thermodynamic equilibrium analysis was
  performed on the spectra of the observed stars. A 3D-NLTE analysis
  was performed to derive the lithium abundance of star #3416. <BR />
  Results: Star #3416 is super Li-rich with A(Li) = 3.75 dex. The lack
  of <SUP>6</SUP>Li enrichment (<SUP>6</SUP>Li/<SUP>7</SUP>Li &lt;
  2%), the low carbon isotopic ratio (<SUP>12</SUP>C/<SUP>13</SUP>C =
  14 ± 3), and the lack of evidence for radial velocity variation
  or enhanced rotational velocity (vsini = 2.8 km s<SUP>-1</SUP>)
  all suggest that lithium production has occurred in this star
  through the Cameron &amp; Fowler mechanism. <BR /> Conclusions:
  We identified a super Li-rich core helium-burning, red-clump star
  in an open cluster. Internal production is the most likely cause
  of the observed enrichment. Given the expected short duration of a
  star's Li-rich phase, enrichment is likely to have occurred at the
  red clump or in the immediately preceding phases, namely during the
  He-flash at the tip of the red giant branch (RGB) or while ascending
  the brightest portion of the RGB. <P />Based on observations made
  with ESO Telescopes at the La Silla Paranal Observatory under program
  ID 088.D-0045(A).Appendix A is available in electronic form at <A
  href="http://www.aanda.org/10.1051/0004-6361/201323348/olm">http://www.aanda.org</A>

---------------------------------------------------------
Title: Detection of magnetic fields in central stars of planetary
    nebulae
Authors: Todt, H.; Steffen, M.; Hubrig, S.; Schöller, M.; Hamann,
   W. -R.; Sandin, C.; Schönberner, D.
2014apn6.confE.103T    Altcode:
  Magnetic fields may play an essential role in shaping planetary
  nebulae. However, convincing evidence for the presence of magnetic
  fields on their central stars is still missing. We obtained
  low-resolution polarimetric spectra with FORS2 for twelve central
  stars. Their nebulae cover different morphologies, comprising two round
  nebulae, seven elliptical nebulae, and three bipolar nebulae. For
  one central star, which has a bipolar nebula, we clearly detect a
  weak magnetic field of the order of 100 Gauss. Interestingly, the
  central star exhibits a hydrogen-free, Wolf-Rayet type spectrum. For
  a few further stars in our sample we find marginal evidence for weak
  magnetic fields. The detection of magnetic fields via polarimetry
  strongly depends on the quality of the observations, and on the type of
  the line spectrum. We perform careful estimates of the error margins,
  using statistical tests and Monte-Carlo simulations, which confirm
  the significance of the detection reported here.

---------------------------------------------------------
Title: 3D modeling of stellar atmospheres and the impact on the
    understanding of the reliability of elemental abundances in stars
    as tracers of galactic chemical evolution
Authors: Ludwig, H. -G.; Steffen, M.; Bonifacio, P.; Caffau, E.;
   Kučinskas, A.; Freytag, B.
2014IAUS..298..343L    Altcode:
  We present a critical review of the construction of 3D model atmospheres
  with emphasis on modeling challenges. We discuss the basic physical
  processes which give rise to the effects which set 3D models apart
  from 1D standard models. We consider elemental abundances derived
  from molecular features, and the determination of the microturbulence
  with 3D models. The examples serve as illustration of the limitations
  inherent to 1D, however, also to 3D modeling. We find that 3D models
  can provide constraints on the microturbulence parameter, and predict
  substantial corrections for abundances derived from molecular species.

---------------------------------------------------------
Title: 3D Model Atmospheres of White Dwarfs
Authors: Tremblay, Pier-Emmanuel; Ludwig, H.; Steffen, M.; Freytag, B.
2014AAS...22331507T    Altcode:
  We present the first grid of 3D model atmospheres for
  hydrogen-atmosphere (DA) white dwarfs. These CO5BOLD
  radiation-hydrodynamics simulations, unlike the previous 1D
  calculations, do not rely on the mixing-length theory for the
  treatment of convection. The simulations have been employed to compute
  model spectra and we compared our improved Balmer line profiles to
  spectroscopic data from the Sloan Digital Sky Survey and the White
  Dwarf Catalog. The 3D surface gravities are found to be as much as
  0.3 dex lower than the values derived from 1D models. The white dwarfs
  with a radiative and a convective atmosphere have derived mean masses
  that are the same within 0.01 Msun with our new models, in much better
  agreement with our understanding of stellar evolution.

---------------------------------------------------------
Title: The first generations of stars
Authors: Caffau, E.; Gallagher, A.; Bonifacio, P.; Cayrel, R.;
   Christlieb, N.; Clark, P. C.; Francois, P.; Glover, S.; Klessen,
   R. S.; Koch, A.; Ludwig, H. G.; Monaco, L.; Plez, B.; Sbordone, L.;
   Spite, M.; Spite, F.; Steffen, M.; Zaggia, S.
2014nic..confE..53C    Altcode: 2014PoS...204E..53C
  No abstract at ADS

---------------------------------------------------------
Title: A hydrodynamical study of multiple-shell planetary
nebulae. III. Expansion properties and internal kinematics: Theory
    versus observation
Authors: Schönberner, D.; Jacob, R.; Lehmann, H.; Hildebrandt, G.;
   Steffen, M.; Zwanzig, A.; Sandin, C.; Corradi, R. L. M.
2014AN....335..378S    Altcode: 2014arXiv1404.0391S
  We present the result of a study on the expansion properties and
  internal kinematics of round/elliptical planetary nebulae of the
  Milky Way disk, the halo, and of the globular cluster M 15. The
  purpose of this study is to considerably enlarge the small sample of
  nebulae with precisely determined expansion properties (Schönberner
  et al. \cite{SJSPCA.05}). To this aim, we selected a representative
  sample of objects with different evolutionary stages and metallicities
  and conducted high-resolution échelle spectroscopy. In most cases
  we succeeded in detecting the weak signals from the outer nebular
  shell which are attached to the main line emission from the bright
  nebular rim. Next to the measurement of the motion of the rim gas by
  decomposition of the main line components into Gaussians, we were
  able to measure separately, for most objects for the first time,
  the gas velocity immediately behind the leading shock of the shell,
  i.e. the post-shock velocity. We more than doubled the number of objects
  for which the velocities of both rim and shell are known and confirm
  that the overall expansion of planetary nebulae is accelerating with
  time. There are, however, differences between the expansion behaviour of
  the shell and the rim: The post-shock velocity is starting at values as
  low as around 20 km s<SUP>-1</SUP> for the youngest nebulae, just above
  the AGB wind velocity of ∼ 10-15 km s<SUP>-1</SUP>, and is reaching
  values of about 40 km s<SUP>-1</SUP> for the nebulae around hotter
  central stars. Contrarily, the rim matter is at first decelerated
  below the typical AGB-wind velocity and remains at about 5-10 km
  s<SUP>-1</SUP> for a while until finally a typical flow velocity of
  up to 30 km s<SUP>-1</SUP> is reached. This observed distinct velocity
  evolution of both rim and shell is explained by radiation-hydrodynamics
  simulations, at least qualitatively: It is due to the ever changing
  stellar radiation field and wind-wind interaction together with the
  varying density profile ahead of the leading shock during the progress
  of evolution. The wind-wind interaction works on the rim dynamics while
  the radiation field and upstream density gradient is responsible for the
  shell dynamics. Because of these time-dependent boundary conditions,
  a planetary nebula will never evolve into a simple self-similar
  expansion. Also the metal-poor objects behave as theory predicts:
  The post-shock velocities are higher and the rim flow velocities are
  equal or even lower compared to disk objects at similar evolutionary
  stage. The old nebula around low-luminosity central stars contained
  in our sample expand still fast and are dominated by reionisation. We
  detected, for the first time, in some objects an asymmetric expansion
  behaviour: The relative expansions between rim and shell appear to
  be different for the receding and approaching parts of the nebular
  envelope. <P />Based partly on observations obtained at the European
  Southern Observatory, Paranal, Chile (ESO programme No. 077.D-0652).

---------------------------------------------------------
Title: TOPoS: chemical study of extremely metal-poor stars.
Authors: Caffau, E.; Sbordone, L.; Bonifacio, P.; Cayrel, R.;
   Christlieb, N.; Clark, P.; François, P.; Glover, S.; Klessen, R.;
   Koch, A.; Ludwig, H. -G.; Monaco, L.; Plez, B.; Spite, F.; Spite,
   M.; Steffen, M.; Zaggia, S.
2014MmSAI..85..222C    Altcode:
  The extremely metal-poor (EMP) stars hold in their atmospheres
  the fossil record of the chemical composition of the early phases
  of the Galactic evolution. The chemical analysis of such objects
  provides important constraints on these early phases. EMP stars
  are very rare objects; to dig them out, large amounts of data have
  to be processed. With an automatic procedure, we analysed objects
  with colours of Turn-Off stars from the Sloan Digital Sky Survey to
  select a sample of good candidate EMP stars. In the latest years,
  we observed a sample of these candidates with X-Shooter and UVES,
  and we have an ongoing ESO large programme to use these spectrographs
  to observe EMP stars. I will report here the results on metallicity
  and Strontium abundance. <P />Based on observations obtained at ESO
  Paranal Observatory, programme 189.D-0165(A)

---------------------------------------------------------
Title: 6Li/7Li isotopic ratio in the most metal-poor binary
    CS22876-032
Authors: Gonzalez-Hernandez, J.; Caffau, E.; Ludwig, H. G.; Bonifacio,
   P.; Steffen, M.; Monaco, L.; Cayrel, R.
2014nic..confE..23G    Altcode: 2014PoS...204E..23G
  No abstract at ADS

---------------------------------------------------------
Title: Isotope spectroscopy
Authors: Caffau, E.; Steffen, M.; Bonifacio, P.; Ludwig, H. -G.;
   Monaco, L.; Lo Curto, G.; Kamp, I.
2014AN....335...59C    Altcode: 2013arXiv1310.6058C
  The measurement of isotopic ratios provides a privileged insight
  both into nucleosynthesis and into the mechanisms operating in
  stellar envelopes, such as gravitational settling. In this article,
  we give a few examples of how isotopic ratios can be determined from
  high-resolution, high-quality stellar spectra. We consider examples of
  the lightest elements, H and He, for which the isotopic shifts are very
  large and easily measurable, and examples of heavier elements for which
  the determination of isotopic ratios is more difficult. The presence
  of <SUP>6</SUP>Li in the stellar atmospheres causes a subtle extra
  depression in the red wing of the <SUP>7</SUP>Li 670.7 nm doublet which
  can only be detected in spectra of the highest quality. But even with
  the best spectra, the derived <SUP>6</SUP>Li abundance can only be as
  good as the synthetic spectra used for their interpretation. It is now
  known that 3D non-LTE modelling of the lithium spectral line profiles
  is necessary to account properly for the intrinsic line asymmetry,
  which is produced by convective flows in the atmospheres of cool stars,
  and can mimic the presence of <SUP>6</SUP>Li. We also discuss briefly
  the case of the carbon isotopic ratio in metal-poor stars, and provide a
  new determination of the nickel isotopic ratios in the solar atmosphere.

---------------------------------------------------------
Title: TOPoS. I. Survey design and analysis of the first sample
Authors: Caffau, E.; Bonifacio, P.; Sbordone, L.; François, P.;
   Monaco, L.; Spite, M.; Plez, B.; Cayrel, R.; Christlieb, N.; Clark,
   P.; Glover, S.; Klessen, R.; Koch, A.; Ludwig, H. -G.; Spite, F.;
   Steffen, M.; Zaggia, S.
2013A&A...560A..71C    Altcode: 2013arXiv1310.6963C
  Context. The metal-weak tail of the metallicity distribution function
  (MDF) of the Galactic Halo stars contains crucial information on the
  formation mode of the first generation of stars. To determine this
  observationally, it is necessary to observe large numbers of extremely
  metal-poor stars. <BR /> Aims: We present here the Turn-Off Primordial
  Stars survey (TOPoS) that is conducted as an ESO Large Programme at the
  VLT. This project has four main goals: (i) to understand the formation
  of low-mass stars in a low-metallicity gas: determine the metal-weak
  tail of the halo MDF below [M/H] = -3.5; in particular, we aim at
  determining the critical metallicity, that is the lowest metallicity
  sufficient for the formation of low-mass stars; (ii) to determine in
  extremely metal-poor stars the relative abundances of the elements that
  are the signature of the massive first stars; (iii) to determine the
  trend of the lithium abundance at the time when the Galaxy formed; and
  (iv) to derive the fraction of C-enhanced extremely metal-poor stars
  with respect to normal extremely metal-poor stars. The large number of
  stars observed in the SDSS provides a good sample of candidate stars
  at extremely low metallicity. <BR /> Methods: Candidates with turn-off
  colours down to magnitude g = 20 were selected from the low-resolution
  spectra of SDSS by means of an automated procedure. X-Shooter has the
  potential of performing the necessary follow-up spectroscopy, providing
  accurate metallicities and abundance ratios for several key elements
  for these stars. <BR /> Results: We present here the stellar parameters
  of the first set of stars. The nineteen stars range in iron abundance
  between -4.1 and -2.9 dex relative to the Sun. Two stars have a high
  radial velocity and, according to our estimate of their kinematics,
  appear to be marginally bound to the Galaxy and are possibly accreted
  from another galaxy. <P />Based on observations obtained at ESO Paranal
  Observatory, GTO programme 189.D-0165(A).

---------------------------------------------------------
Title: Spectroscopic analysis of DA white dwarfs with 3D model
    atmospheres
Authors: Tremblay, P. -E.; Ludwig, H. -G.; Steffen, M.; Freytag, B.
2013A&A...559A.104T    Altcode: 2013arXiv1309.0886T
  We present the first grid of mean three-dimensional (3D) spectra for
  pure-hydrogen (DA) white dwarfs based on 3D model atmospheres. We use
  CO<SUP>5</SUP>BOLD radiation-hydrodynamics 3D simulations instead of the
  mixing-length theory for the treatment of convection. The simulations
  cover the effective temperature range of 6000 &lt; T<SUB>eff</SUB>
  (K) &lt; 15 000 and the surface gravity range of 7 &lt; log g &lt;
  9 where the large majority of DAs with a convective atmosphere
  are located. We rely on horizontally averaged 3D structures (over
  constant Rosseland optical depth) to compute ⟨3D⟩ spectra. It
  is demonstrated that our ⟨3D⟩ spectra can be smoothly connected
  to their 1D counterparts at higher and lower T<SUB>eff</SUB> where
  the 3D effects are small. Analytical functions are provided in order
  to convert spectroscopically determined 1D effective temperatures
  and surface gravities to 3D atmospheric parameters. We apply our
  improved models to well studied spectroscopic data sets from the
  Sloan Digital Sky Survey and the White Dwarf Catalog. We confirm
  that the so-called high-log g problem is not present when employing
  ⟨3D⟩ spectra and that the issue was caused by inaccuracies in
  the 1D mixing-length approach. The white dwarfs with a radiative
  and a convective atmosphere have derived mean masses that are
  the same within ~0.01 M<SUB>⊙</SUB>, in much better agreement
  with our understanding of stellar evolution. Furthermore, the 3D
  atmospheric parameters are in better agreement with independent
  T<SUB>eff</SUB> and log g values from photometric and parallax
  measurements. <P />Appendices are only available in electronic form
  at <A href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: Three-dimensional hydrodynamical CO<SUP>5</SUP>BOLD model
    atmospheres of red giant stars. III. Line formation in the atmospheres
    of giants located close to the base of the red giant branch
Authors: Dobrovolskas, V.; Kučinskas, A.; Steffen, M.; Ludwig,
   H. -G.; Prakapavičius, D.; Klevas, J.; Caffau, E.; Bonifacio, P.
2013A&A...559A.102D    Altcode: 2013arXiv1310.7791D
  <BR /> Aims: We utilize state-of-the-art three-dimensional (3D)
  hydrodynamical and classical 1D stellar model atmospheres to study
  the influence of convection on the formation properties of various
  atomic and molecular spectral lines in the atmospheres of four red
  giant stars, located close to the base of the red giant branch, RGB
  (T<SUB>eff</SUB> ≈ 5000 K, log g = 2.5), and characterized by four
  different metallicities, [M/H] = 0.0, -1.0, -2.0, -3.0. <BR /> Methods:
  The role of convection in the spectral line formation is assessed with
  the aid of abundance corrections, i.e., the differences in abundances
  predicted for a given equivalent width of a particular spectral line
  with the 3D and 1D model atmospheres. The 3D hydrodynamical and
  classical 1D model atmospheres used in this study were calculated
  with the CO<SUP>5</SUP>BOLD and 1D LHD codes, respectively. Identical
  atmospheric parameters, chemical composition, equation of state, and
  opacities were used with both codes, therefore allowing a strictly
  differential analysis of the line formation properties in the 3D and 1D
  models. <BR /> Results: We find that for lines of certain neutral atoms,
  such as Mg i, Ti i, Fe i, and Ni i, the abundance corrections strongly
  depend both on the metallicity of a given model atmosphere and the line
  excitation potential, χ. While abundance corrections for all lines of
  both neutral and ionized elements tend to be small at solar metallicity
  (≤±0.1 dex), for lines of neutral elements with low ionization
  potential and low-to-intermediate χ they quickly increase with
  decreasing metallicity, reaching in their extremes -0.6 to -0.8 dex. In
  all such cases the large abundance corrections are due to horizontal
  temperature fluctuations in the 3D hydrodynamical models. Lines of
  neutral elements with higher ionization potentials (E<SUB>ion</SUB>
  ≳ 10 eV) generally behave very similarly to lines of ionized elements
  characterized by low ionization potentials (E<SUB>ion</SUB> ≲ 6
  eV). In the latter case, the abundance corrections are small (generally,
  ≤±0.1 dex) and are caused by approximately equal contributions
  from the horizontal temperature fluctuations and differences between
  the temperature profiles in the 3D and 1D model atmospheres. Abundance
  corrections of molecular lines are very sensitive to the metallicity of
  the underlying model atmosphere and may be larger (in absolute value)
  than ~-0.5 dex at [M/H] = -3.0 (~-1.5 dex in the case of CO). At fixed
  metallicity and excitation potential, the abundance corrections show
  little variation within the wavelength range studied here, 400-1600
  nm. We also find that an approximate treatment of scattering in the
  3D model calculations (i.e., ignoring the scattering opacity in the
  outer, optically thin, atmosphere) leads to abundance corrections
  that are altered by less than ~0.1 dex, both for atomic and molecular
  (CO) lines, with respect to the model where scattering is treated as
  true absorption throughout the entire atmosphere, with the largest
  differences for the resonance and low-excitation lines. <P />Appendices
  and Figs. 3, 5, 6, 8, 9, 11 are available in electronic form at <A
  href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: The evolution of planetary nebulae. VIII. True expansion
    rates and visibility times
Authors: Jacob, R.; Schönberner, D.; Steffen, M.
2013A&A...558A..78J    Altcode: 2013arXiv1307.6189J
  Context. The visibility time of planetary nebulae (PNe) in stellar
  systems is an essential quantity for estimating the size of a PN
  population in the context of general population studies. For instance,
  it enters directly into the PN death rate determination. <BR /> Aims:
  The basic ingredient for determining visibility times is the typical
  nebular expansion velocity, as a suited average over all PN sizes
  of a PN population within a certain volume or stellar system. The
  true expansion speed of the outer nebular edge of a PN is, however,
  not accessible by spectroscopy - a difficulty that we surmount by
  radiation-hydrodynamics modelling. <BR /> Methods: We first discuss
  the definition of the PN radius and possible differences between
  the observable PN radius and its physical counterpart, the position
  of the leading shock of the nebular shell. We also compare the Hα
  surface-brightness evolution predicted by our radiation-hydrodynamics
  models with the recent Hα surface-brightness radius calibration of Frew
  (2008, Ph.D. Thesis, Macquarie University, Australia) and find excellent
  agreement. We then carefully investigate the existing spectroscopic data
  on nebular expansion velocities for a local PN sample with objects up
  to a distance of 2 kpc with well-defined round/elliptical shapes. We
  evaluate, by means of our radiation-hydrodynamics models, how these
  observed expansion velocities must be corrected in order to get the
  true expansion speed of the outer nebular edge. <BR /> Results: We find
  a mean true expansion velocity of 42 km s<SUP>-1</SUP>, i.e. nearly
  twice as high as the commonly adopted value to date. Accordingly,
  the time for a PN to expand to a radius of, say 0.9 pc, is only
  21 000 ± 5000 years. This visibility time of a PN holds for all
  central star masses since a nebula does not become extinct as the
  central star fades. There is, however, a dependence on metallicity
  in the sense that the visibility time becomes shorter for lower
  nebular metal content. <BR /> Conclusions: These statements on the
  visibility time only hold for volume-limited samples. Extragalactic
  samples that contain spatially unresolved nebulae are flux limited,
  and in this case the visibility time directly depends on the limiting
  magnitude of the survey. To reach a visibility time of 21 000 years,
  the survey must reach about 7 mag below the bright cut-off of the
  planetary nebula luminosity function. With the higher expansion
  rate of PNe derived here we determined their local death-rate
  density as (1.4 ± 0.5) × 10<SUP>-12</SUP> PN pc<SUP>-3</SUP>
  yr<SUP>-1</SUP>, using the local PN density advocated by Frew
  (2008). <P />Appendix A is available in electronic form at <A
  href="http://www.aanda.org">http://www.aanda.org</A>Dedicated to the
  memory of Volker Weidemann who died on March 14, 2012, at the age of
  87 years.

---------------------------------------------------------
Title: Granulation properties of giants, dwarfs, and white dwarfs
    from the CIFIST 3D model atmosphere grid
Authors: Tremblay, P. -E.; Ludwig, H. -G.; Freytag, B.; Steffen, M.;
   Caffau, E.
2013A&A...557A...7T    Altcode: 2013arXiv1307.2810T
  Three-dimensional model atmospheres for giants, dwarfs, and white
  dwarfs, computed with the CO5BOLD code and part of the CIFIST grid,
  have been used for spectroscopic and asteroseismic studies. Unlike
  existing plane-parallel 1D structures, these simulations predict
  the spatially and temporally resolved emergent intensity so that
  granulation can be analysed, which provides insights on how convective
  energy transfer operates in stars. The wide range of atmospheric
  parameters of the CIFIST 3D simulations (3600 &lt; T<SUB>eff</SUB>
  (K) &lt; 13 000 and 1 &lt; log g &lt; 9) allows the comparison of
  convective processes in significantly different environments. We
  show that the relative intensity contrast is correlated with both
  the Mach and Péclet numbers in the photosphere. The horizontal size
  of granules varies between 3 and 10 times the local pressure scale
  height, with a tight correlation between the factor and the Mach
  number of the flow. Given that convective giants, dwarfs, and white
  dwarfs cover the same range of Mach and Péclet numbers, we conclude
  that photospheric convection operates in a very similar way in those
  objects. <P />Table 1 and Appendix A are available in electronic form
  at <A href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: Evaluating local correlation tracking using CO5BOLD simulations
    of solar granulation
Authors: Verma, M.; Steffen, M.; Denker, C.
2013A&A...555A.136V    Altcode: 2013arXiv1305.6033V
  Context. Flows on the solar surface are intimately linked to
  solar activity, and local correlation tracking (LCT) is one of the
  standard techniques for capturing the dynamics of these processes by
  cross-correlating solar images. However, the link between contrast
  variations in successive images to the underlying plasma motions has
  to be quantitatively confirmed. <BR /> Aims: Radiation hydrodynamics
  simulations of solar granulation (e.g., CO<SUP>5</SUP>BOLD) provide
  access to both the wavelength-integrated, emergent continuum intensity
  and the three-dimensional velocity field at various heights in the
  solar atmosphere. Thus, applying LCT to continuum images yields
  horizontal proper motions, which are then compared to the velocity
  field of the simulated (non-magnetic) granulation. In this study, we
  evaluate the performance of an LCT algorithm previously developed for
  bulk-processing Hinode G-band images, establish it as a quantitative
  tool for measuring horizontal proper motions, and clearly work out
  the limitations of LCT or similar techniques designed to track optical
  flows. <BR /> Methods: Horizontal flow maps and frequency distributions
  of the flow speed were computed for a variety of LCT input parameters
  including the spatial resolution, the width of the sampling window,
  the time cadence of successive images, and the averaging time used to
  determine persistent flow properties. Smoothed velocity fields from
  the hydrodynamics simulation at three atmospheric layers (log τ = -1,
  0, and +1) served as a point of reference for the LCT results. <BR />
  Results: LCT recovers many of the granulation properties, e.g., the
  shape of the flow speed distributions, the relationship between mean
  flow speed and averaging time, and also - with significant smoothing
  of the simulated velocity field - morphological features of the
  flow and divergence maps. However, the horizontal proper motions are
  grossly underestimated by as much as a factor of three. The LCT flows
  match best the flows deeper in the atmosphere at log τ = +1. <BR />
  Conclusions: Despite the limitations of optical flow techniques, they
  are a valuable tool in describing horizontal proper motions on the Sun,
  as long as the results are not taken at face value but with a proper
  understanding of the input parameter space and the limitations inherent
  to the algorithm. <P />Movies are available in electronic form at <A
  href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: The Intensity-Velocity Phase Spectra of Evanescent Oscillations
    and Acoustic Sources
Authors: Severino, G.; Straus, T.; Oliviero, M.; Steffen, M.; Fleck, B.
2013SoPh..284..297S    Altcode: 2012SoPh..tmp..295S
  There are three major issues in modeling solar evanescent oscillations:
  the variation of the intensity [I]-velocity [V] phase difference of
  p-modes close to the base of photosphere; the existence of a plateau
  of negative I-V phase differences below and between the ridges of the
  low-frequency p-modes; the explanation of the I-V cross-spectra of
  the evanescent oscillations. We present new interpretations for the
  first two issues, based on modeling intensity fluctuations taking steep
  temperature gradients, opacity, and non-adiabatic cooling into account.

---------------------------------------------------------
Title: The photospheric solar oxygen project. II. Non-concordance
    of the oxygen abundance derived from two forbidden lines
Authors: Caffau, E.; Ludwig, H. -G.; Malherbe, J. -M.; Bonifacio,
   P.; Steffen, M.; Monaco, L.
2013A&A...554A.126C    Altcode: 2013arXiv1305.1763C
  Context. In the Sun, the two forbidden [O i] lines at 630 and 636 nm
  were previously found to provide discrepant oxygen abundances. <BR
  /> Aims: We investigate whether this discrepancy is peculiar to the
  Sun or whether it is also observed in other stars. <BR /> Methods:
  We make use of high-resolution, high signal-to-noise ratio spectra of
  four dwarf to turn-off stars, five giant stars, and one sub-giant star
  observed with THEMIS, HARPS, and UVES to investigate the coherence of
  the two lines. <BR /> Results: The two lines provide oxygen abundances
  that are consistent, within observational errors, in all the giant
  stars examined by us. On the other hand, for the two dwarf stars for
  which a measurement was possible, for Procyon, and for the sub-giant
  star Capella, the 636 nm line provides systematically higher oxygen
  abundances, as already seen for the Sun. <BR /> Conclusions: The
  only two possible reasons for the discrepancy are a serious error
  in the oscillator strength of the Ni i line blending the 630 nm line
  or the presence of an unknown blend in the 636 nm line, which makes
  the feature stronger. The CN lines blending the 636 nm line cannot
  be responsible for the discrepancy. The Ca i autoionisation line, on
  the red wing of which the 636 nm line is formed, is not well modelled
  by our synthetic spectra. However, a better reproduction of this line
  would result in even higher abundances from the 636 nm, thus increasing
  the discrepancy. <P />Based on observations collected at ESO Paranal
  Observatory, Programme 182.D-5053(A).

---------------------------------------------------------
Title: Pure-hydrogen 3D model atmospheres of cool white dwarfs
Authors: Tremblay, P. -E.; Ludwig, H. -G.; Steffen, M.; Freytag, B.
2013A&A...552A..13T    Altcode: 2013arXiv1302.2013T
  A sequence of pure-hydrogen CO5BOLD 3D model atmospheres of DA white
  dwarfs is presented for a surface gravity of log g = 8 and effective
  temperatures from 6000 to 13 000 K. We show that convective properties,
  such as flow velocities, characteristic granulation size and intensity
  contrast of the granulation patterns, change significantly over this
  range. We demonstrate that these 3D simulations are not sensitive to
  numerical parameters unlike the 1D structures that considerably depend
  on the mixing-length parameters. We conclude that 3D spectra can be used
  directly in the spectroscopic analyses of DA white dwarfs. We confirm
  the result of an earlier preliminary study that 3D model spectra provide
  a much better characterization of the mass distribution of white dwarfs
  and that shortcomings of the 1D mixing-length theory are responsible
  for the spurious high-log g determinations of cool white dwarfs. In
  particular, the 1D theory is unable to account for the cooling effect
  of the convective overshoot in the upper atmospheres.

---------------------------------------------------------
Title: Detection of Diffuse X-Ray Emission from Planetary Nebulae
    with Nebular O VI
Authors: Ruiz, N.; Chu, Y. -H.; Gruendl, R. A.; Guerrero, M. A.;
   Jacob, R.; Schönberner, D.; Steffen, M.
2013ApJ...767...35R    Altcode: 2013arXiv1302.3886R
  The presence of O VI ions can be indicative of plasma temperatures of
  a few ×10<SUP>5</SUP> K that are expected in heat conduction layers
  between the hot shocked stellar wind gas at several 10<SUP>6</SUP>
  K and the cooler (10<SUP>4</SUP> K) nebular gas of planetary nebulae
  (PNe). We have used FUSE observations of PNe to search for nebular O
  VI emission or absorption as a diagnostic of the conduction layer to
  ensure the presence of hot interior gas. Three PNe showing nebular O VI,
  namely IC 418, NGC 2392, and NGC 6826, have been selected for Chandra
  observations and diffuse X-ray emission is indeed detected in each of
  these PNe. Among the three, NGC 2392 has peculiarly high diffuse X-ray
  luminosity and plasma temperature compared with those expected from
  its stellar wind's mechanical luminosity and terminal velocity. The
  limited effects of heat conduction on the plasma temperature of a hot
  bubble at the low terminal velocity of the stellar wind of NGC 2392 may
  partially account for its high plasma temperature, but the high X-ray
  luminosity needs to be powered by processes other than the observed
  stellar wind, probably the presence of an unseen binary companion of the
  central star of the PN (CSPN) of NGC 2392. We have compiled relevant
  information on the X-ray, stellar, and nebular properties of PNe with
  a bubble morphology and found that the expectations of bubble models
  including heat conduction compare favorably with the present X-ray
  observations of hot bubbles around H-rich CSPNe, but have notable
  discrepancies for those around H-poor [WR] CSPNe. We note that PNe
  with more massive central stars can produce hotter plasma and higher
  X-ray surface brightness inside central hot bubbles.

---------------------------------------------------------
Title: Three-dimensional hydrodynamical CO<SUP>5</SUP>BOLD model
    atmospheres of red giant stars. II. Spectral line formation in the
    atmosphere of a giant located near the RGB tip
Authors: Kučinskas, A.; Steffen, M.; Ludwig, H. -G.; Dobrovolskas,
   V.; Ivanauskas, A.; Klevas, J.; Prakapavičius, D.; Caffau, E.;
   Bonifacio, P.
2013A&A...549A..14K    Altcode: 2012arXiv1211.7313K
  <BR /> Aims: We investigate the role of convection in the formation of
  atomic and molecular lines in the atmosphere of a red giant star. For
  this purpose we study the formation properties of spectral lines that
  belong to a number of astrophysically important tracer elements,
  including neutral and singly ionized atoms (Li I, N I, O I, Na I,
  Mg I, Al I, Si I, Si II, S I, K I, Ca I, Ca II, Ti I, Ti II, Cr I,
  Cr II, Mn I, Fe I, Fe II, Co I, Ni I, Zn I, Sr II, Ba II, and Eu II),
  and molecules (CH, CO, C<SUB>2</SUB>, NH, CN, and OH). <BR /> Methods:
  We focus our investigation on a prototypical red giant located close to
  the red giant branch (RGB) tip (T<SUB>eff</SUB> = 3660 K, log g = 1.0,
  [M/H] = 0.0). We used two types of model atmospheres, 3D hydrodynamical
  and classical 1D, calculated with the CO<SUP>5</SUP>BOLD and LHD
  stellar atmosphere codes, respectively. Both codes share the same
  atmospheric parameters, chemical composition, equation of state,
  and opacities, which allowed us to make a strictly differential
  comparison between the line formation properties predicted in 3D and
  1D. The influence of convection on the spectral line formation was
  assessed with the aid of 3D-1D abundance corrections, which measure
  the difference between the abundances of chemical species derived
  with the 3D hydrodynamical and 1D classical model atmospheres. <BR
  /> Results: We find that convection plays a significant role in
  the spectral line formation in this particular red giant. The
  derived 3D-1D abundance corrections rarely exceed ± 0.1 dex when
  lines of neutral atoms and molecules are considered, which is in
  line with the previous findings for solar-metallicity red giants
  located on the lower RGB. The situation is different with lines that
  belong to ionized atoms, or to neutral atoms with high ionization
  potential. In both cases, the corrections for high-excitation lines
  (χ &gt; 8 eV) may amount to Δ<SUB>3D-1D</SUB> ~ -0.4 dex. The
  3D-1D abundance corrections generally show a significant wavelength
  dependence; in most cases they are smaller in the near-infrared, at
  1600-2500 nm. <P />Appendices are available in electronic form at <A
  href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: First steps with CO5BOLD using HLLMHD and PP reconstruction .
Authors: Steiner, O.; Rajaguru, S. P.; Vigeesh, G.; Steffen, M.;
   Schaffenberger, W.; Freytag, B.
2013MSAIS..24..100S    Altcode:
  We report on first experiences with real-life applications using
  the MHD-module of CO5BOLD together with the piecewise parabolic
  reconstruction scheme and present preliminary results of stellar
  magnetic models with T<SUB>eff</SUB> = 4000 K to T<SUB>eff</SUB> =
  5770 K.

---------------------------------------------------------
Title: Granulation in DA white dwarfs from CO5BOLD 3D model
    atmospheres
Authors: Tremblay, P. -E.; Ludwig, H. -G.; Freytag, B.; Steffen, M.
2013MSAIS..24...61T    Altcode:
  Time-dependent 3D simulations of pure-hydrogen DA white dwarf
  atmospheres have been computed in recent years. Synthetic Balmer lines
  spectra drawn from these radiation-hydrodynamics (RHD) simulations
  have been shown to predict surface gravities significantly lower than
  the standard 1D models, in much better agreement with the expectation
  that white dwarfs cool at constant mass. We have now computed a grid
  of CO5BOLD pure-hydrogen 3D model atmospheres for surface gravities
  from log g = 7 to log g = 8.5 and effective temperatures from 6000 to
  13,000 K. Over this range, we observe a significant variation of the
  intensity contrast of the surface granulation patterns, which indicates
  the strength of the 3D effects. Furthermore, the size and appearance
  of granules are also varying considerably. An explanation of these
  behaviours can lead to a better understanding of the physical processes
  responsible for the energy transfer in white dwarf atmospheres.

---------------------------------------------------------
Title: Micro- and macroturbulence predictions from CO5BOLD 3D stellar
    atmospheres .
Authors: Steffen, M.; Caffau, E.; Ludwig, H. -G.
2013MSAIS..24...37S    Altcode: 2013arXiv1306.4307S
  We present an overview of the current status of our efforts to derive
  the microturbulence and macroturbulence parameters (xi_mic and xi_mac)
  from the CIFIST grid of CO5BOLD 3D model atmospheres as a function
  of the basic stellar parameters T_{eff}, log g, and [M/H]. The latest
  results for the Sun and Procyon show that the derived microturbulence
  parameter depends significantly on the numerical resolution of the
  underlying 3D simulation, confirming that `low-resolution' models tend
  to underestimate the true value of xi_mic . Extending the investigation
  to 12 further simulations with different T_{eff}, log g, and [M/H],
  we obtain a first impression of the predicted trend of xi_mic over the
  Hertzsprung-Russell diagram: in agreement with empirical evidence,
  microturbulence increases towards higher effective temperature and
  lower gravity. The metallicity dependence of xi_mic must be interpreted
  with care, since it also reflects the deviation between the 1D and 3D
  photospheric temperature stratifications that increases systematically
  towards lower [M/H].

---------------------------------------------------------
Title: Spectral line asymmetries in the metal-poor red giant HD
122563: CO<SUP>5</SUP>BOLD predictions versus observations
Authors: Klevas, J.; Ludwig, A. Kučinskas H. -G.; Bonifacio, P.;
   Steffen, M.
2013MSAIS..24...78K    Altcode: 2013arXiv1303.6838K
  We study the influence of convection on the asymmetries and Doppler
  shifts of Fe I spectral lines in the metal-poor red giant HD 122563. To
  this end, we compute theoretical Fe I line shifts and line bisectors
  using 3D hydrodynamical model atmosphere of HD 122563 calculated with
  the CO<SUP>5</SUP>BOLD code. We then make a detailed comparison of the
  theoretical line shifts and bisectors with those derived from the high
  quality HARPS spectrum of HD 122563 taken from the ESO Science Archive
  Facility (R=115 000, average signal-to-noise ratio, S/N ≈ 310). In
  general, we find a good agreement between the theoretically predicted
  and observed Doppler shifts of Fe I line cores, with somewhat larger
  discrepancies seen in the case of weaker (equivalent width W&lt;5
  pm) and stronger lines (W&gt;11 pm). Both observed and theoretical
  coreshifts cover a range between 0 and -1 km/s, with increasingly
  stronger blueshifts for weaker lines and slight hints of a coreshift
  dependence on wavelength. Theoretical bisectors reproduce the observed
  ones reasonably well too, however, theoretical bisectors of the weak red
  (lambda &gt; 600 nm) Fe I lines have blueshifts that are by up to ∼200
  m/s larger than observed. The obtained results therefore suggest that
  the current CO<SUP>5</SUP>BOLD models are capable of reproducing the
  large-scale velocity fields in the atmosphere of HD 122563 sufficiently
  well. Nevertheless, further efforts are needed in order to understand
  the physical reasons behind the discrepancies in theoretical predictions
  and observed properties of the weakest and strongest Fe I lines.

---------------------------------------------------------
Title: The influence of convection on the atmospheric structures
    and observable properties of red giant stars.
Authors: Kučinskas, A.; Ludwig, H. -G.; Steffen, M.; Dobrovolskas,
   V.; Klevas, J.; Prakapavičius, D.; Caffau, E.; Bonifacio, P.
2013MSAIS..24...68K    Altcode: 2013arXiv1305.3441K
  During the recent years significant progress has been made in the
  modeling of red giant atmospheres with the aid of 3D hydrodynamical
  model atmosphere codes. In this contribution we provide an overview of
  selected results obtained in this context by utilizing 3D hydrodynamical
  CO<SUP>5</SUP>BOLD stellar model atmospheres. Hydrodynamical simulations
  show that convective motions lead to significant differences in the
  atmospheric structures of red giants with respect to those predicted by
  the classical 1D model atmospheres. Results of these simulations also
  show that in certain cases 1D models fail to reproduce even the average
  properties of the 3D hydrodynamical models, such as P-T profiles. Large
  horizontal temperature fluctuations in the 3D model atmospheres, as well
  as differences between the temperature profiles of the average xtmean
  {3D} and 1D models, lead to large discrepancies in the strengths of
  spectral lines predicted by the 3D and 1D model atmospheres. This is
  especially important in models at lowest metallicities ([M/H]&lt;-2.0)
  where the 3D-1D abundance differences may reach (or even exceed) -0.6
  dex for lines of neutral atoms and molecules. We also discuss several
  simplifications and numerical aspects involved in the present 3D
  hydrodynamical modeling of red giant atmospheres, and briefly address
  several issues where urgent progress may be needed.

---------------------------------------------------------
Title: Molecular bands in extremely metal-poor stars: Granulation
    effects
Authors: Bonifacio, P.; Caffau, E.; Ludwig, H. -G.; Spite, M.; Plez,
   B.; Steffen, M.; Spite, F.
2013MSAIS..24..138B    Altcode: 2013arXiv1305.2065B
  The bands of diatomic molecules are important abundance indicators,
  especially in metal-poor stars, where they are still measurable in
  metallicity regimes where the atomic lines of their constituting
  metallic elements have become vanishingly small. In order to use
  them for abundance determinations it is imperative to understand the
  formation of these bands. In this contribution we report on our results
  obtained using CO^5{BOLD} hydrodynamical simulations. Some effects
  that are qualitatively different from what found in 1D computations
  are highlighted. Due to the large number of lines that form the bands,
  their spectrum synthesis is computationally challenging. We discuss
  some of the computational strategies we employed to parallelise the
  computation and possible future developments.

---------------------------------------------------------
Title: Opacities in CO<SUP>5</SUP>BOLD
Authors: Ludwig, H. -G.; Steffen, M.
2013MSAIS..24...53L    Altcode:
  We describe the present treatment of the frequency-dependence of
  the radiative transfer in CO<SUP>5</SUP>BOLD. This mostly refers to
  the way opacities are binned into groups. We discuss the basic ideas
  behind the Opacity Binning Method, give some details of the practical
  implementation in CO<SUP>5</SUP>BOLD, and point to some issues where
  improvements are needed.

---------------------------------------------------------
Title: Oxygen spectral line synthesis: 3D non-LTE with
    CO<SUP>5</SUP>BOLD hydrodynamical model atmospheres.
Authors: Prakapavičius, D.; Steffen, M.; Kučinskas, A.; Ludwig,
   H. -G.; Freytag, B.; Caffau, E.; Cayrel, R.
2013MSAIS..24..111P    Altcode: 2013arXiv1303.2016P
  In this work we present first results of our current project aimed at
  combining the 3D hydrodynamical stellar atmosphere approach with non-LTE
  (NLTE) spectral line synthesis for a number of key chemical species. We
  carried out a full 3D-NLTE spectrum synthesis of the oxygen IR 777 nm
  triplet, using a modified and improved version of our NLTE3D package to
  calculate departure coefficients for the atomic levels of oxygen in a
  CO<SUP>5</SUP>BOLD 3D hydrodynamical solar model atmosphere. Spectral
  line synthesis was subsequently performed with the Linfor3D code. In
  agreement with previous studies, we find that the lines of the
  oxygen triplet produce deeper cores under NLTE conditions, due to
  the diminished line source function in the line forming region. This
  means that the solar oxygen IR 777 nm lines should be stronger in NLTE,
  leading to negative 3D NLTE-LTE abundance corrections. Qualitatively
  this result would support previous claims for a relatively low solar
  oxygen abundance. Finally, we outline several further steps that need
  to be taken in order to improve the physical realism and numerical
  accuracy of our current 3D-NLTE calculations.

---------------------------------------------------------
Title: 3D Model Atmospheres of DA White Dwarfs
Authors: Tremblay, P. -E.; Ludwig, H. -G.; Steffen, M.; Freytag, B.
2013ASPC..469..155T    Altcode:
  The spectroscopically determined surface gravities of cool
  hydrogen-atmosphere DA white dwarfs are significantly higher than
  the mean value of log g ∼ 8 found for hotter objects with radiative
  atmospheres (T<SUB>eff</SUB> &gt; 13000 K). It was recently suggested
  that a problem with the treatment of convective energy transport in
  the 1D mixing-length theory was the explanation for this high-log
  g problem. We have now computed a grid of pure-hydrogen 3D model
  atmospheres with the CO<SUP>5</SUP>BOLD code for surface gravities
  from log g = 7 to 8.5 and effective temperatures from 6000 to 13000
  K. Over this range, the intensity contrast of the surface granulation
  pattern, which describes the strength of the 3D effects, is varying
  significantly. We confirm the result of an earlier investigation that
  3D model spectra provide a much better characterization of the mass
  distribution of cool white dwarfs.

---------------------------------------------------------
Title: Magnetic field detection in the bright A0-type supergiant
    HD 92207
Authors: Hubrig, S.; Schöller, M.; Kholtygin, A. F.; González,
   J. F.; Kharchenko, N. V.; Steffen, M.
2012A&A...546L...6H    Altcode:
  Context. Recent developments in observational techniques and theories
  revealed the potential significance of magnetic fields for stellar
  structure, evolution, and circumstellar environment. At present,
  the distribution of magnetic field strengths in massive stars from
  the zero-age main sequence to more evolved stages, which would shed
  light on the origin of the magnetic field, has not been studied. <BR />
  Aims: We searched for the presence of a magnetic field in the visually
  brightest early A-type supergiant HD 92207. <BR /> Methods: Observations
  were obtained using the low-resolution spectropolarimetric mode of
  FORS 2 (FOcal Reducer low dispersion Spectrograph) mounted on the 8 m
  Antu telescope of the VLT. For the mean longitudinal magnetic field
  measurements, we applied a linear regression analysis in two ways:
  using only the absorption hydrogen Balmer lines or using the entire
  spectrum including all available absorption lines. <BR /> Results: A
  mean longitudinal magnetic field at a significance level of more than
  3σ was detected in two out of three observations distributed over
  about one year. It is one of the rare cases where a field of about
  a few hundred Gauss is detected in an early A-type supergiant. All
  line profiles in the spectra of HD 92207 undergo distinct variations
  in radial velocities and intensities, probably caused by previously
  detected non-radial pulsations. <P />Based on observations obtained at
  the European Southern Observatory (Prgs. 074.D-0008(B), 078.D-0330(A),
  087.D-0049(A), and 088.D-0425(A)).

---------------------------------------------------------
Title: The role of heat conduction to the formation of [WC]-type
    planetary nebulae
Authors: Sandin, Christer; Steffen, Matthias; Jacob, Ralf;
   Schönberner, Detlef; Rühling, Ute; Hamann, Wolf-Rainer; Todt, Helge
2012IAUS..283..494S    Altcode:
  X-ray observations of young Planetary Nebulæ (PNe) have revealed
  diffuse emission in extended regions around both H-rich and
  H-deficient central stars. In order to also reproduce physical
  properties of H-deficient objects, we have, at first, extended our
  time-dependent radiation-hydrodynamic models with heat conduction
  for such conditions. Here we present some of the important physical
  concepts, which determine how and when a hot wind-blown bubble
  forms. In this study we have had to consider the, largely unknown,
  evolution of the CSPN, the slow (AGB) wind, the fast hot-CSPN wind,
  and the chemical composition. The main conclusion of our work is that
  heat conduction is needed to explain X-ray properties of wind-blown
  bubbles also in H-deficient objects.

---------------------------------------------------------
Title: Planetary nebula abundance determinations: A view from 1D-RHD
    simulations
Authors: Jacob, Ralf; Sandin, Christer; Schönberner, Detlef; Steffen,
   Matthias
2012IAUS..283..398J    Altcode:
  In the last years (metallicity-dependent) radiation-hydrodynamics
  simulations have become a powerful tool to understand the
  formation and evolution of PNe in terms of simple morphologies and
  kinematics. Contrary to photoionization models, with their ad-hoc
  assumptions on structure and physics, the RHD models are self-consistent
  with respect to their density distribution, velocity field, chemical
  composition, and stellar evolution. We use our models as simple proxies
  for real PNe and investigate the reliability of common abundance
  determination methods, which are based on either plasma diagnostics
  or static photoionization (PI) models.

---------------------------------------------------------
Title: Modeling the diffuse X-ray emission of planetary nebulae with
    different chemical composition
Authors: Steffen, Matthias; Sandin, Christer; Jacob, Ralf;
   Schönberner, Detlef
2012IAUS..283..215S    Altcode: 2011arXiv1109.6355S
  Based on time-dependent radiation-hydrodynamics simulations of the
  evolution of Planetary Nebulae (PNe), we have carried out a systematic
  parameter study to address the non-trivial question of how the diffuse
  X-ray emission of PNe with closed central cavities is expected to depend
  on the evolutionary state of the nebula, the mass of the central star,
  and the metallicity of stellar wind and circumstellar matter. We have
  also investigated how the model predictions depend on the treatment of
  thermal conduction at the interface between the central `hot bubble'
  and the `cool' inner nebula, and compare the results with recent X-ray
  observations. Our study includes models whose properties resemble
  the extreme case of PNe with Wolf-Rayet type central stars. Indeed,
  such models are found to produce the highest X-ray luminosities.

---------------------------------------------------------
Title: The Chandra X-Ray Survey of Planetary Nebulae (ChanPlaNS):
    Probing Binarity, Magnetic Fields, and Wind Collisions
Authors: Kastner, J. H.; Montez, R., Jr.; Balick, B.; Frew, D. J.;
   Miszalski, B.; Sahai, R.; Blackman, E.; Chu, Y. -H.; De Marco, O.;
   Frank, A.; Guerrero, M. A.; Lopez, J. A.; Rapson, V.; Zijlstra, A.;
   Behar, E.; Bujarrabal, V.; Corradi, R. L. M.; Nordhaus, J.; Parker,
   Q. A.; Sandin, C.; Schönberner, D.; Soker, N.; Sokoloski, J. L.;
   Steffen, M.; Ueta, T.; Villaver, E.
2012AJ....144...58K    Altcode: 2012arXiv1204.6055K
  We present an overview of the initial results from the Chandra Planetary
  Nebula Survey (ChanPlaNS), the first systematic (volume-limited)
  Chandra X-Ray Observatory survey of planetary nebulae (PNe) in the
  solar neighborhood. The first phase of ChanPlaNS targeted 21 mostly
  high-excitation PNe within ~1.5 kpc of Earth, yielding four detections
  of diffuse X-ray emission and nine detections of X-ray-luminous point
  sources at the central stars (CSPNe) of these objects. Combining these
  results with those obtained from Chandra archival data for all (14)
  other PNe within ~1.5 kpc that have been observed to date, we find an
  overall X-ray detection rate of ~70% for the 35 sample objects. Roughly
  50% of the PNe observed by Chandra harbor X-ray-luminous CSPNe, while
  soft, diffuse X-ray emission tracing shocks—in most cases, "hot
  bubbles"—formed by energetic wind collisions is detected in ~30%; five
  objects display both diffuse and point-like emission components. The
  presence (or absence) of X-ray sources appears correlated with PN
  density structure, in that molecule-poor, elliptical nebulae are
  more likely to display X-ray emission (either point-like or diffuse)
  than molecule-rich, bipolar, or Ring-like nebulae. All but one of the
  point-like CSPNe X-ray sources display X-ray spectra that are harder
  than expected from hot (~100 kK) central stars emitting as simple
  blackbodies; the lone apparent exception is the central star of the
  Dumbbell nebula, NGC 6853. These hard X-ray excesses may suggest a high
  frequency of binary companions to CSPNe. Other potential explanations
  include self-shocking winds or PN mass fallback. Most PNe detected as
  diffuse X-ray sources are elliptical nebulae that display a nested
  shell/halo structure and bright ansae; the diffuse X-ray emission
  regions are confined within inner, sharp-rimmed shells. All sample
  PNe that display diffuse X-ray emission have inner shell dynamical
  ages &lt;~ 5 × 10<SUP>3</SUP> yr, placing firm constraints on the
  timescale for strong shocks due to wind interactions in PNe. The
  high-energy emission arising in such wind shocks may contribute to the
  high excitation states of certain archetypical "hot bubble" nebulae
  (e.g., NGC 2392, 3242, 6826, and 7009).

---------------------------------------------------------
Title: Ablation and Wind Mass-Loading in the Born-Again Planetary
    Nebula A 30
Authors: Guerrero, Martín A.; Chu, You-Hua; Hamann, Wolf-Rainer;
   Oskinova, Lidia; Schönberner, Detlef; Todt, Helge; Steffen, Matthias;
   Ruiz, Nieves; Gruendl, Robert A.; Blair, William P.
2012IAUS..283..378G    Altcode:
  We present XMM-Newton and Chandra observations of the born-again
  planetary nebula A 30. These X-ray observations reveal a bright
  unresolved source at the position of the central star whose X-ray
  luminosity exceeds by far the model expectations for photospheric
  emission and for shocks within the stellar wind. We suggest that
  a “born-again hot bubble” may be responsible for this X-ray
  emission. Diffuse X-ray emission associated with the petal-like
  features and one of the H-poor knots seen in the optical is also
  found. The weakened emission of carbon lines in the spectrum of the
  diffuse emission can be interpreted as the dilution of stellar wind
  by mass-loading or as the detection of material ejected during a very
  late thermal pulse.

---------------------------------------------------------
Title: X-ray spectra of wind-driven bubbles with chemical gradients
Authors: Jacob, Ralf; Sandin, Christer; Schönberner, Detlef; Steffen,
   Matthias
2012IAUS..283..396J    Altcode:
  As a tool helping to interpret diffuse X-ray emission of PNe, and as a
  supplement to our RHD simulations, we have started to construct a grid
  of theoretical X-ray spectra of wind-blown bubbles with temperature and
  density profiles according to thermal conduction theory. We investigate
  how the X-ray spectra depend on chemical composition (e.g. H-rich
  vs. H-deficient) and how temperature and abundance determinations
  reflect gradients of temperature and chemical composition within
  the bubbles. These synthetic models shall allow to quickly perform
  detailed parameter studies without the need for dedicated hydrodynamical
  simulations. We report on ideas and goals.

---------------------------------------------------------
Title: On the internal kinematics of PNe
Authors: Jacob, Ralf; Schönberner, Detlef; Lehmann, Holger; Zwanzig,
   Alena; Sandin, Christer; Steffen, Matthias
2012IAUS..283..400J    Altcode:
  Our sample of round/elliptical double-shell PNe around central stars
  (CSs) with H-rich surface chemistry covers all evolutionary phases
  across the HRD. By means of high-resolution and high-S/N spectra we
  determine bulk matter velocities of the inner wind-driven rims and
  the maximum (= post-shock) gas velocities of the surrounding thermally
  expanding shells. Studying the details of the internal kinematics allows
  a look at processes of PN formation and at PN expansion history helping,
  for instance, to determine expansion distances.

---------------------------------------------------------
Title: Rebirth of X-Ray Emission from the Born-again Planetary
    Nebula A30
Authors: Guerrero, M. A.; Ruiz, N.; Hamann, W. -R.; Chu, Y. -H.;
   Todt, H.; Schönberner, D.; Oskinova, L.; Gruendl, R. A.; Steffen,
   M.; Blair, W. P.; Toalá, J. A.
2012ApJ...755..129G    Altcode: 2012arXiv1202.4463G
  The planetary nebula A30 is believed to have undergone a very late
  thermal pulse resulting in the ejection of knots of hydrogen-poor
  material. Using multi-epoch Hubble Space Telescope images, we have
  detected the angular expansion of these knots and derived an age of
  850<SUP>+280</SUP> <SUB>- 150</SUB> yr. To investigate the spectral
  and spatial properties of the soft X-ray emission detected by ROSAT,
  we have obtained Chandra and XMM-Newton deep observations of A30. The
  X-ray emission from A30 can be separated into two components: a point
  source at the central star and diffuse emission associated with the
  hydrogen-poor knots and the cloverleaf structure inside the nebular
  shell. To help us assess the role of the current stellar wind in
  powering this X-ray emission, we have determined the stellar parameters
  and wind properties of the central star of A30 using a non-LTE model fit
  to its optical and UV spectra. The spatial distribution and spectral
  properties of the diffuse X-ray emission are highly suggestive that
  it is generated by the post-born-again and present fast stellar winds
  interacting with the hydrogen-poor ejecta of the born-again event. This
  emission can be attributed to shock-heated plasma, as the hydrogen-poor
  knots are ablated by the stellar winds, under which circumstances
  the efficient mass loading of the present fast stellar wind raises
  its density and damps its velocity to produce the observed diffuse
  soft X-rays. Charge transfer reactions between the ions of the stellar
  winds and material of the born-again ejecta have also been considered
  as a possible mechanism for the production of diffuse X-ray emission,
  and upper limits on the expected X-ray production by this mechanism
  have been derived. The origin of the X-ray emission from the central
  star of A30 is puzzling: shocks in the present fast stellar wind and
  photospheric emission can be ruled out, while the development of a new,
  compact hot bubble confining the fast stellar wind seems implausible.

---------------------------------------------------------
Title: A primordial star in the heart of the Lion
Authors: Caffau, E.; Bonifacio, P.; François, P.; Spite, M.; Spite,
   F.; Zaggia, S.; Ludwig, H. -G.; Steffen, M.; Mashonkina, L.; Monaco,
   L.; Sbordone, L.; Molaro, P.; Cayrel, R.; Plez, B.; Hill, V.; Hammer,
   F.; Randich, S.
2012A&A...542A..51C    Altcode: 2012arXiv1203.2607C
  Context. The discovery and chemical analysis of extremely metal-poor
  stars permit a better understanding of the star formation of the first
  generation of stars and of the Universe emerging from the Big Bang. <BR
  /> Aims: We report the study of a primordial star situated in the centre
  of the constellation Leo (SDSS J102915+172927). <BR /> Methods: The
  star, selected from the low-resolution spectrum of the Sloan Digital
  Sky Survey, was observed at intermediate (with X-Shooter at VLT) and
  at high spectral resolution (with UVES at VLT). The stellar parameters
  were derived from the photometry. The standard spectroscopic analysis
  based on 1D ATLAS models was completed by applying 3D and non-LTE
  corrections. <BR /> Results: An iron abundance of [Fe/H ] = -4.89 makes
  SDSS J102915+172927 one of the lowest [Fe/H] stars known. However,
  the absence of measurable C and N enhancements indicates that it has
  the lowest metallicity, Z ≤ 7.40 × 10<SUP>-7</SUP> (metal-mass
  fraction), ever detected. No oxygen measurement was possible. <BR />
  Conclusions: The discovery of SDSS J102915+172927 highlights that
  low-mass star formation occurred at metallicities lower than previously
  assumed. Even lower metallicity stars may yet be discovered, with a
  chemical composition closer to the composition of the primordial gas
  and of the first supernovae. <P />Based on observations obtained at ESO
  Paranal Observatory, GTO programme 086.D-0094 and programme 286.D-5045.

---------------------------------------------------------
Title: Excitation of Slow-Modes in Network Magnetic Elements
Authors: Kato, Y.; Steiner, O.; Steffen, M.; Suematsu, Y.
2012ASPC..455..237K    Altcode:
  From radiation magnetohydrodynamic (RMHD) simulations of the solar
  atmosphere we have found a new mechanism for the excitation of
  longitudinal slow modes within magnetic flux concentrations. It is
  found that the convective downdrafts in the immediate surroundings of
  magnetic elements are responsible for the excitation of slow modes. The
  coupling between the external downdraft and the plasma motion internal
  to the flux concentration is mediated by the inertial forces of the
  downdraft that act on the magnetic flux concentration. These forces
  pump the internal atmosphere in the downward direction, which entails
  a fast downflow in the photospheric and chromospheric layers of the
  magnetic element. Subsequent to the transient pumping phase, the
  atmosphere rebounds, causing a slow mode traveling along the magnetic
  flux concentration in the upward direction and developing into a shock
  wave in chromospheric heights, possibly capable of producing some kind
  of dynamic fibril. This event occurs recurrently. We compare the power
  spectra of the temperature and velocity of the flux-sheet atmosphere
  to the corresponding spectra of the unmagnetized atmosphere.

---------------------------------------------------------
Title: Using Hubble Space Telescope Images to Test Theoretical Models
    of Planetary Nebulae
Authors: Braxton, Kelsey M.; Balick, B.; Jacob, R.; Steffen, M.;
   Schonberner, D.
2012AAS...22043110B    Altcode:
  Classical ionization models that predict the ionization structure
  of planetary nebulae generally assume constant gas density (or
  a central void and constant density) in the shell. More recently,
  Steffen, Jacob, Schoenberner (2005, A&amp;A, 441, 573) have computed
  fully consistent one-dimensional radiation hydrodynamic ionization
  models (RHI models) with realistic stellar winds and evolving central
  stars. Their numerical results offer concrete predictions concerning
  the projected three-dimensional shapes of simple round and elliptical
  PNe. A first glance at their models shows them to be a superior way of
  modeling ionization structures in realistic PNe. We present high-spatial
  resolution and carefully flux calibrated images of PNe selected in
  Halpha, [OIII], and [NII] as well as the ratios [OIII]/Halpha and
  [NII]/Halpha in order to test the predictions of the RHI models. These
  were obtained uniformly and at the same epoch using the WFPC2 camera on
  the Hubble Space Telescope. Some of the targets are ionization bounded
  and others are density bounded. In the future these images will be
  compared to the models in detail. At this point we note many of the
  common features--some of them unexpected--that the models must explain.

---------------------------------------------------------
Title: LTE Model Atmospheres: MARCS, ATLAS and CO5BOLD
Authors: Bonifacio, P.; Caffau, E.; Ludwig, H. -G.; Steffen, M.
2012IAUS..282..213B    Altcode:
  In this talk, we review the basic assumptions and physics covered
  by classical 1D LTE model atmospheres. We will focus on ATLAS and
  MARCS models of F-G-K stars and describe what resources are available
  through the web, both in terms of codes and model-atmosphere grids. We
  describe the advances made in hydrodynamical simulations of convective
  stellar atmospheres with the CO<SUP>5</SUP>BOLD code and what grids
  and resources are available, with a prospect of what will be available
  in the near future.

---------------------------------------------------------
Title: The Gaia-ESO Public Spectroscopic Survey
Authors: Gilmore, G.; Randich, S.; Asplund, M.; Binney, J.; Bonifacio,
   P.; Drew, J.; Feltzing, S.; Ferguson, A.; Jeffries, R.; Micela, G.;
   Negueruela, I.; Prusti, T.; Rix, H. -W.; Vallenari, A.; Alfaro, E.;
   Allende-Prieto, C.; Babusiaux, C.; Bensby, T.; Blomme, R.; Bragaglia,
   A.; Flaccomio, E.; François, P.; Irwin, M.; Koposov, S.; Korn, A.;
   Lanzafame, A.; Pancino, E.; Paunzen, E.; Recio-Blanco, A.; Sacco,
   G.; Smiljanic, R.; Van Eck, S.; Walton, N.; Aden, D.; Aerts, C.;
   Affer, L.; Alcala, J. -M.; Altavilla, G.; Alves, J.; Antoja, T.;
   Arenou, F.; Argiroffi, C.; Asensio Ramos, A.; Bailer-Jones, C.;
   Balaguer-Nunez, L.; Bayo, A.; Barbuy, B.; Barisevicius, G.; Barrado
   y Navascues, D.; Battistini, C.; Bellas Velidis, I.; Bellazzini, M.;
   Belokurov, V.; Bergemann, M.; Bertelli, G.; Biazzo, K.; Bienayme, O.;
   Bland-Hawthorn, J.; Boeche, C.; Bonito, S.; Boudreault, S.; Bouvier,
   J.; Brandao, I.; Brown, A.; de Bruijne, J.; Burleigh, M.; Caballero,
   J.; Caffau, E.; Calura, F.; Capuzzo-Dolcetta, R.; Caramazza, M.;
   Carraro, G.; Casagrande, L.; Casewell, S.; Chapman, S.; Chiappini,
   C.; Chorniy, Y.; Christlieb, N.; Cignoni, M.; Cocozza, G.; Colless,
   M.; Collet, R.; Collins, M.; Correnti, M.; Covino, E.; Crnojevic,
   D.; Cropper, M.; Cunha, M.; Damiani, F.; David, M.; Delgado, A.;
   Duffau, S.; Edvardsson, B.; Eldridge, J.; Enke, H.; Eriksson, K.;
   Evans, N. W.; Eyer, L.; Famaey, B.; Fellhauer, M.; Ferreras, I.;
   Figueras, F.; Fiorentino, G.; Flynn, C.; Folha, D.; Franciosini,
   E.; Frasca, A.; Freeman, K.; Fremat, Y.; Friel, E.; Gaensicke, B.;
   Gameiro, J.; Garzon, F.; Geier, S.; Geisler, D.; Gerhard, O.; Gibson,
   B.; Gomboc, A.; Gomez, A.; Gonzalez-Fernandez, C.; Gonzalez Hernandez,
   J.; Gosset, E.; Grebel, E.; Greimel, R.; Groenewegen, M.; Grundahl,
   F.; Guarcello, M.; Gustafsson, B.; Hadrava, P.; Hatzidimitriou, D.;
   Hambly, N.; Hammersley, P.; Hansen, C.; Haywood, M.; Heber, U.; Heiter,
   U.; Held, E.; Helmi, A.; Hensler, G.; Herrero, A.; Hill, V.; Hodgkin,
   S.; Huelamo, N.; Huxor, A.; Ibata, R.; Jackson, R.; de Jong, R.;
   Jonker, P.; Jordan, S.; Jordi, C.; Jorissen, A.; Katz, D.; Kawata,
   D.; Keller, S.; Kharchenko, N.; Klement, R.; Klutsch, A.; Knude,
   J.; Koch, A.; Kochukhov, O.; Kontizas, M.; Koubsky, P.; Lallement,
   R.; de Laverny, P.; van Leeuwen, F.; Lemasle, B.; Lewis, G.; Lind,
   K.; Lindstrom, H. P. E.; Lobel, A.; Lopez Santiago, J.; Lucas, P.;
   Ludwig, H.; Lueftinger, T.; Magrini, L.; Maiz Apellaniz, J.; Maldonado,
   J.; Marconi, G.; Marino, A.; Martayan, C.; Martinez-Valpuesta, I.;
   Matijevic, G.; McMahon, R.; Messina, S.; Meyer, M.; Miglio, A.;
   Mikolaitis, S.; Minchev, I.; Minniti, D.; Moitinho, A.; Momany, Y.;
   Monaco, L.; Montalto, M.; Monteiro, M. J.; Monier, R.; Montes, D.;
   Mora, A.; Moraux, E.; Morel, T.; Mowlavi, N.; Mucciarelli, A.; Munari,
   U.; Napiwotzki, R.; Nardetto, N.; Naylor, T.; Naze, Y.; Nelemans, G.;
   Okamoto, S.; Ortolani, S.; Pace, G.; Palla, F.; Palous, J.; Parker, R.;
   Penarrubia, J.; Pillitteri, I.; Piotto, G.; Posbic, H.; Prisinzano,
   L.; Puzeras, E.; Quirrenbach, A.; Ragaini, S.; Read, J.; Read, M.;
   Reyle, C.; De Ridder, J.; Robichon, N.; Robin, A.; Roeser, S.; Romano,
   D.; Royer, F.; Ruchti, G.; Ruzicka, A.; Ryan, S.; Ryde, N.; Santos,
   N.; Sanz Forcada, J.; Sarro Baro, L. M.; Sbordone, L.; Schilbach, E.;
   Schmeja, S.; Schnurr, O.; Schoenrich, R.; Scholz, R. -D.; Seabroke, G.;
   Sharma, S.; De Silva, G.; Smith, M.; Solano, E.; Sordo, R.; Soubiran,
   C.; Sousa, S.; Spagna, A.; Steffen, M.; Steinmetz, M.; Stelzer, B.;
   Stempels, E.; Tabernero, H.; Tautvaisiene, G.; Thevenin, F.; Torra,
   J.; Tosi, M.; Tolstoy, E.; Turon, C.; Walker, M.; Wambsganss, J.;
   Worley, C.; Venn, K.; Vink, J.; Wyse, R.; Zaggia, S.; Zeilinger, W.;
   Zoccali, M.; Zorec, J.; Zucker, D.; Zwitter, T.; Gaia-ESO Survey Team
2012Msngr.147...25G    Altcode:
  The Gaia-ESO Public Spectroscopic Survey has begun and will obtain high
  quality spectroscopy of some 100000 Milky Way stars, in the field and
  in open clusters, down to magnitude 19, systematically covering all the
  major components of the Milky Way. This survey will provide the first
  homogeneous overview of the distributions of kinematics and chemical
  element abundances in the Galaxy. The motivation, organisation and
  implementation of the Gaia-ESO Survey are described, emphasising the
  complementarity with the ESA Gaia mission. Spectra from the very first
  observing run of the survey are presented.

---------------------------------------------------------
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.

---------------------------------------------------------
Title: Simulations of stellar convection with CO5BOLD
Authors: Freytag, B.; Steffen, M.; Ludwig, H. -G.; Wedemeyer-Böhm,
   S.; Schaffenberger, W.; Steiner, O.
2012JCoPh.231..919F    Altcode: 2011arXiv1110.6844F
  High-resolution images of the solar surface show a granulation
  pattern of hot rising and cooler downward-sinking material - the
  top of the deep-reaching solar convection zone. Convection plays a
  role for the thermal structure of the solar interior and the dynamo
  acting there, for the stratification of the photosphere, where most
  of the visible light is emitted, as well as for the energy budget of
  the spectacular processes in the chromosphere and corona. Convective
  stellar atmospheres can be modeled by numerically solving the coupled
  equations of (magneto)hydrodynamics and non-local radiation transport
  in the presence of a gravity field. The CO5BOLD code described in this
  article is designed for so-called "realistic" simulations that take
  into account the detailed microphysics under the conditions in solar
  or stellar surface layers (equation-of-state and optical properties of
  the matter). These simulations indeed deserve the label "realistic"
  because they reproduce the various observables very well - with only
  minor differences between different implementations. The agreement
  with observations has improved over time and the simulations are now
  well-established and have been performed for a number of stars. Still,
  severe challenges are encountered when it comes to extending these
  simulations to include ideally the entire star or substellar object:
  the strong stratification leads to completely different conditions in
  the interior, the photosphere, and the corona. Simulations have to cover
  spatial scales from the sub-granular level to the stellar diameter and
  time scales from photospheric wave travel times to stellar rotation
  or dynamo cycle periods. Various non-equilibrium processes have to be
  taken into account. Last but not least, realistic simulations are based
  on detailed microphysics and depend on the quality of the input data,
  which can be the actual accuracy limiter. This article provides an
  overview of the physical problem and the numerical solution and the
  capabilities of CO5BOLD, illustrated with a number of applications.

---------------------------------------------------------
Title: <SUP>6</SUP>Li detection in metal-poor stars: can 3D model
    atmospheres solve the second lithium problem?
Authors: Steffen, M.; Cayrel, R.; Caffau, E.; Bonifacio, P.; Ludwig,
   H. -G.; Spite, M.
2012MSAIS..22..152S    Altcode: 2012arXiv1206.2239S
  The presence of <SUP>6</SUP>Li in the atmospheres of metal-poor
  halo stars is usually inferred from the detection of a subtle extra
  depression in the red wing of the <SUP>7</SUP>Li doublet line at
  670.8 nm. However, as pointed out recently by \cite{Cayrel2007},
  the intrinsic line asymmetry caused by convective flows in the
  photospheres of cool stars is almost indistinguishable from the
  asymmetry produced by a weak <SUP>6</SUP>Li blend on a (presumed)
  symmetric <SUP>7</SUP>Li profile. Previous determinations of the
  <SUP>6</SUP>Li/ <SUP>7</SUP>Li isotopic ratio based on 1D model
  atmospheres, ignoring the convection-induced line asymmetry, must
  therefore be considered as upper limits. By comparing synthetic
  1D LTE and 3D non-LTE line profiles of the <SUP>i</SUP>Li 670.8 nm
  feature, we quantify the differential effect of the convective line
  asymmetry on the derived <SUP>6</SUP>Li abundance as a function of
  effective temperature, gravity, and metallicity. As expected, we
  find that the asymmetry effect systematically reduces the resulting
  <SUP>6</SUP>Li/<SUP>7</SUP>Li ratios. Depending on the stellar
  parameters, the 3D-1D offset in <SUP>6</SUP>Li/<SUP>7</SUP>Li ranges
  between -0.005 and -0.020. When this purely theoretical correction is
  taken into account for the \cite{A2006} sample of stars, the number of
  significant <SUP>6</SUP>Li detections decreases from 9 to 5 (2sigma
  criterion), or from 5 to 2 (3sigma criterion). <P />We also present
  preliminary results of a re-analysis of high-resolution, high S/N
  spectra of individual metal-poor turn-off stars, to see whether the
  second Lithium problem actually disappears when accounting properly for
  convection and non-LTE line formation in 3D stellar atmospheres. Out
  of 8 stars, HD 84937 seems to be the only significant (2sigma )
  detection of <SUP>6</SUP>Li. In view of our results, the existence of
  a <SUP>6</SUP>Li plateau appears questionable.

---------------------------------------------------------
Title: 3D Model Atmospheres of Red Giant Stars
Authors: Ludwig, Hans-Günter; Steffen, Matthias
2012ASSP...26..125L    Altcode: 2011arXiv1108.4554L; 2012rgps.book..125L
  We provide a brief overview of the modelling of the atmospheres of
  red giant stars with the 3D radiation-hydrodynamics code CO5BOLD. We
  emphasize aspects where 3D modelling provides additional insight
  beyond standard hydrostatic 1D models, and comment on present modelling
  challenges.

---------------------------------------------------------
Title: Radiation-Hydrodynamics Simulations of Cool Stellar and
    Substellar Atmospheres
Authors: Freytag, B.; Allard, F.; Ludwig, H. -G.; Homeier, D.;
   Steffen, M.
2011ASPC..448..855F    Altcode: 2011csss...16..855F
  In the atmospheres of brown dwarfs, not only molecules but much
  larger and heavier "dust" particles can form. The latter should sink
  under the influence of gravity into deeper layers and vanish from the
  atmosphere, clearing it from condensable material. However, observed
  spectra can only be reproduced by models assuming the presence of dust
  and its resulting greenhouse effect in the visible layers. Apparently,
  hydrodynamical mixing can counteract the gravitational settling. We
  present new 2D and 3D radiation-hydrodynamics simulations with CO5BOLD
  of the upper part of the convection zone and the atmosphere of cool
  stars and brown dwarfs in a range of temperatures and gravities
  that enable the formation of dust clouds in the visible layers. We
  find that the differences between 2D and 3D models are remarkably
  small. Lowering the gravity has a somewhat similar effect on the surface
  intensity contrast as increasing the effective temperature. The biggest
  uncertainties of the simulations come from approximations made in the
  description of the dust chemistry. Global circulation and rotation
  likely play an important role.

---------------------------------------------------------
Title: Radiation Hydrodynamics Simulations of Dust Clouds in the
    Atmospheres of Substellar Objects
Authors: Freytag, B.; Allard, F.; Homeier, D.; Ludwig, H.; Steffen, M.
2011ASPC..450..125F    Altcode:
  The temperature structure and the motions in the atmospheres of cool
  stars are affected by the underlying convection zone. The radiation
  hydrodynamics code CO5BOLD has been developed to simulate (small patches
  of the) convective surface layers of these stars. Updated opacity tables
  based on PHOENIX data and a description for the formation, destruction,
  advective transport, and settling of dust have made the code fit to
  handle the conditions in brown dwarf atmospheres. Currently, objects
  from 8500 K down to about 900 K have been simulated. Recently, incident
  radiation has been included, allowing simulations with conditions
  found on hot planets. In non-irradiated brown dwarf models we encounter
  mixing by gravity waves and in the cooler models convection within the
  clouds. The qualitative effects of incident radiation are surprisingly
  small, as long as the effective temperature of the object stays well
  below the dust condensation temperature. Beyond that point, there are
  no layers where dust could form, anymore.

---------------------------------------------------------
Title: LTE model atmopsheres MARCS, ATLAS and CO5BOLD
Authors: Bonifacio, Piercarlo; Caffau, Elisabetta; Ludwig,
   Hans-Guenter; Steffen, Matthias
2011arXiv1109.0717B    Altcode:
  In this talk we review the basic assumptions and physics covered by
  classical 1D LTE model atmospheres. We will focus on ATLAS and MARCS
  models of F-G-K stars and describe what resources are available through
  the web, both in terms of codes and model-atmosphere grids. We describe
  the advances made in hydrodynamical simulations of convective stellar
  atmospheres with the CO5BOLD code and what grids and resources are
  available, with a prospect of what will be available in the near future.

---------------------------------------------------------
Title: The Galactic evolution of phosphorus
Authors: Caffau, E.; Bonifacio, P.; Faraggiana, R.; Steffen, M.
2011A&A...532A..98C    Altcode: 2011arXiv1107.2657C
  Context. As a galaxy evolves, its chemical composition changes and
  the abundance ratios of different elements are powerful probes of
  the underlying evolutionary processes. Phosphorous is an element
  whose evolution has remained quite elusive until now, because it is
  difficult to detect in cool stars. The infrared weak P i lines of
  the multiplet 1, at 1050-1082 nm, are the most reliable indicators
  of the presence of phosphorus. The availability of CRIRES at VLT has
  permitted access to this wavelength range in stellar spectra. <BR />
  Aims: We attempt to measure the phosphorus abundance of twenty cool
  stars in the Galactic disk. <BR /> Methods: The spectra are analysed
  with one-dimensional model-atmospheres computed in local thermodynamic
  equilibrium (LTE). The line formation computations are performed
  assuming LTE. <BR /> Results: The ratio of phosphorus to iron behaves
  similarly to sulphur, increasing towards lower metallicity stars. Its
  ratio with respect to sulphur is roughly constant and slightly larger
  than solar, [P/S] = 0.10 ± 0.10. <BR /> Conclusions: We succeed in
  taking an important step towards the understanding of the chemical
  evolution of phosphorus in the Galaxy. However, the observed rise in
  the P/Fe abundance ratio is steeper than predicted by Galactic chemical
  evolution model developed by Kobayashi and collaborators. Phosphorus
  appears to evolve differently from the light odd-Z elements sodium
  and aluminium. The constant value of [P/S] with metallicity implies
  that P production is insensitive to the neutron excess, thus processes
  other than neutron captures operate. We suggest that proton captures on
  <SUP>30</SUP>Si and α captures on <SUP>27</SUP>Al are possibilities
  to investigate. We see no clear distinction between our results for
  stars with planets and stars without any detected planet. <P />Based
  on observations obtained with the CRIRES spectrograph at ESO-VLT Antu
  8.2 m telescope at Paranal, Programme 386.D-0130, P.I. E. Caffau.

---------------------------------------------------------
Title: Excitation of magneto-acoustic waves in network magnetic
    elements
Authors: Kato, Yoshiaki; Steiner, Oskar; Steffen, Matthias; Suematsu,
   Yoshinori
2011IAUS..273..442K    Altcode:
  From radiation magnetohydrodynamic (RMHD) simulations we track the
  temporal evolution of a vertical magnetic flux sheet embedded in a
  two-dimensional non-stationary atmosphere that reaches all the way
  from the upper convection zone to the low chromosphere. Examining its
  temporal behavior near the interface between the convection zone and
  the photosphere, we describe the excitation of propagating longitudinal
  waves within the magnetic element as a result of convective motion in
  its surroundings.

---------------------------------------------------------
Title: Solution to the problem of the surface gravity distribution
    of cool DA white dwarfs from improved 3D model atmospheres
Authors: Tremblay, P. -E.; Ludwig, H. -G.; Steffen, M.; Bergeron,
   P.; Freytag, B.
2011A&A...531L..19T    Altcode: 2011arXiv1106.6007T
  The surface gravities of cool (T<SUB>eff</SUB> &lt; 13 000 K)
  hydrogen-atmosphere DA white dwarfs, determined from spectroscopic
  analyses, are found to be significantly higher than the canonical value
  of log g ~ 8 expected for these stars. It was recently concluded that
  a problem with the treatment of convective energy transport within
  the framework of the mixing-length theory was the most plausible
  explanation for this high-log g problem. We pursue the investigation
  of this discrepancy by computing model spectra of cool convective
  white dwarfs from a small sequence (11 300 K &lt; T<SUB>eff</SUB>
  &lt; 12 800 K) of 3D hydrodynamical model atmospheres, which feature
  a sophisticated treatment of convection and radiative transfer. Our
  approach is to proceed with a differential analysis between 3D and
  standard 1D models. We find that the 3D spectra predict significantly
  lower surface gravities, with corrections of the right amplitude
  as a function of effective temperature to obtain values of log g ~
  8 on average. We conclude that the surface gravity distribution of
  cool convective DA white dwarfs is much closer to that of hotter
  radiative objects when using, for the treatment of the convection,
  3D models instead of the mixing-length framework. <P />Figure 2 is
  available in electronic form at http://www.aanda.org

---------------------------------------------------------
Title: Excitation of Slow Modes in Network Magnetic Elements Through
    Magnetic Pumping
Authors: Kato, Yoshiaki; Steiner, Oskar; Steffen, Matthias; Suematsu,
   Yoshinori
2011ApJ...730L..24K    Altcode: 2011arXiv1102.5164K
  From radiation magnetohydrodynamic simulations of the solar atmosphere,
  we find a new mechanism for the excitation of longitudinal slow modes
  within magnetic flux concentrations. We find that the convective
  downdrafts in the immediate surroundings of magnetic elements are
  responsible for the excitation of slow modes. The coupling between
  the external downdraft and the plasma motion internal to the flux
  concentration is mediated by the inertial forces of the downdraft that
  act on the magnetic flux concentration. These forces, in conjunction
  with the downward movement, pump the internal atmosphere in the
  downward direction, which entails a fast downdraft in the photospheric
  and chromospheric layers of the magnetic element. Subsequent to the
  transient pumping phase, the atmosphere rebounds, causing a slow
  mode traveling along the magnetic flux concentration in the upward
  direction. It develops into a shock wave in chromospheric heights,
  possibly capable of producing some kind of dynamic fibril. We propose
  an observational detection of this process.

---------------------------------------------------------
Title: The solar photospheric abundance of zirconium
Authors: Caffau, E.; Faraggiana, R.; Ludwig, H. -G.; Bonifacio, P.;
   Steffen, M.
2011AN....332..128C    Altcode: 2010arXiv1012.1038C
  Zirconium (Zr), together with strontium and yttrium, is an important
  element in the understanding of the Galactic nucleosynthesis. In
  fact, the triad Sr-Y-Zr constitutes the first peak of s-process
  elements. Despite its general relevance not many studies of the solar
  abundance of Zr were conducted. We derive the zirconium abundance in
  the solar photosphere with the same CO<SUP>5</SUP>BOLD hydrodynamical
  model of the solar atmosphere that we previously used to investigate
  the abundances of C-N-O. We review the zirconium lines available in
  the observed solar spectra and select a sample of lines to determine
  the zirconium abundance, considering lines of neutral and singly
  ionised zirconium. We apply different line profile fitting strategies
  for a reliable analysis of Zr lines that are blended by lines of other
  elements. The abundance obtained from lines of neutral zirconium is very
  uncertain because these lines are commonly blended and weak in the solar
  spectrum. However, we believe that some lines of ionised zirconium are
  reliable abundance indicators. Restricting the set to Zr II lines,
  from the CO<SUP>5</SUP>BOLD 3D model atmosphere we derive A(Zr)
  {=2.62± 0.06}, where the quoted error is the RMS line-to-line scatter.

---------------------------------------------------------
Title: Solar Chemical Abundances Determined with a CO5BOLD 3D Model
    Atmosphere
Authors: Caffau, E.; Ludwig, H. -G.; Steffen, M.; Freytag, B.;
   Bonifacio, P.
2011SoPh..268..255C    Altcode: 2010SoPh..tmp...66C; 2010arXiv1003.1190C
  In the last decade, the photospheric solar metallicity as determined
  from spectroscopy experienced a remarkable downward revision. Part
  of this effect can be attributed to an improvement of atomic data and
  the inclusion of NLTE computations, but also the use of hydrodynamical
  model atmospheres seemed to play a role. This "decrease" with time of
  the metallicity of the solar photosphere increased the disagreement
  with the results from helioseismology. With a CO<SUP>5</SUP>BOLD 3D
  model of the solar atmosphere, the CIFIST team at the Paris Observatory
  re-determined the photospheric solar abundances of several elements,
  among them C, N, and O. The spectroscopic abundances are obtained by
  fitting the equivalent width and/or the profile of observed spectral
  lines with synthetic spectra computed from the 3D model atmosphere. We
  conclude that the effects of granular fluctuations depend on the
  characteristics of the individual lines, but are found to be relevant
  only in a few particular cases. 3D effects are not responsible for
  the systematic lowering of the solar abundances in recent years. The
  solar metallicity resulting from this analysis is Z=0.0153, Z/X=0.0209.

---------------------------------------------------------
Title: Watching planetary nebulae grow with HST
Authors: Balick, B.; Huehnerhoff, J.; Steffen, M.; Schoenberner, D.;
   Hajian, A.; Behr, B. B.
2011apn5.confP..43B    Altcode: 2011apn5.procA..43B
  HST/WFPC2/PC images of PNe spanning over a decade allow secular changes
  in their sharp-edged structures to monitored and compared to the
  predictions of hydrodynamical interacting winds models. We selected a
  sample of 18 simple, bright, and relatively nearby targets for second-
  or third-epoch observations in 2008 using the F502N ([OIII]) and F658N
  ([NII]) filters. All data sets were identically calibrated and compared
  using difference images. About 75% showed signs of expansion (by up to
  1%) and changes in surface brightness (by up to ±5%). In most cases
  the expansions were largely uniform. Exceptions tend to be found in
  ionization fronts at the perimeter of the ionized gas, though NGC6543
  shows signs of nonuniform expansion in its interior as well. Results
  for NGC 2392, 3132, 3242, 3918, and 6543 were presented.

---------------------------------------------------------
Title: On the chemical composition of the metal-poor planetary
    nebula PNG135.9+55.9
Authors: Sandin, C.; Jacob, R.; Schoenberner, D.; Steffen, M.; Roth,
   M. M.
2011apn5.confP..51S    Altcode: 2011apn5.procA..51S
  The metal-poor planetary nebula PN G135.9+55.9 has a particularly-low
  oxygen abundance, that is a matter of an ongoing discussion. We
  report on our recent results of both new accurate observations by
  means of integral field spectroscopy with PMAS, and on the outcome of
  new radiation hydrodynamics models. Our goal with these studies was
  to calculate new abundance estimates. We find that expansion cooling,
  and deviations from thermal equilibrium, become increasingly important
  to the physical structure at metalicities that are as low as in this
  object. The resulting low electron temperatures cause substantial
  deviations in the estimated abundances compared to an approach using
  standard hydrostatic photo-ionization models.

---------------------------------------------------------
Title: The role of thermal conduction in WR-type planetary nebulae
Authors: Sandin, C.; Steffen, M.; Schoenberner, D.; Ruehling, U.;
   Hamann, W. R.
2011apn5.confP..53S    Altcode: 2011apn5.procA..53S
  Thermal conduction plays an important role to the interpretation of
  X-ray spectra of planetary nebulae. Models including this effect so
  far only used a theoretical formulation that assumes a pure hydrogen
  composition. To permit modeling of objects with other compositions,
  such as Wolf-Rayet stars, we have now extended the thermal-conduction
  description in our models. We will present the outcome of our study
  in terms of how these changes affect the new models and the predicted
  X-ray emission spectra.

---------------------------------------------------------
Title: What does the Sun suggest about global oscillation amplitudes
    in solar-like stars?
Authors: Severino, G.; Straus, Th.; Oliviero, M.; Steffen, M.
2010AN....331..896S    Altcode:
  Motivated by the results of CoRoT and based on the solar experience,
  we develop a new stellar scaling law for the intensity-velocity
  amplitude ratio (gain) of resonant oscillations, which is a quantity
  independent of the excitation model. The comparison of our approach
  with observations gives new interesting results for the Sun as a
  star. Moreover, for a sample of three solar-like stars observed
  by CoRoT, we found that our scaling law provides an explanation of
  the low observed luminosity amplitudes which is an alternative to
  non-adiabatic effects.

---------------------------------------------------------
Title: The metal-poor end of the Spite plateau. I. Stellar parameters,
    metallicities, and lithium abundances
Authors: Sbordone, L.; Bonifacio, P.; Caffau, E.; Ludwig, H. -G.;
   Behara, N. T.; González Hernández, J. I.; Steffen, M.; Cayrel, R.;
   Freytag, B.; van't Veer, C.; Molaro, P.; Plez, B.; Sivarani, T.; Spite,
   M.; Spite, F.; Beers, T. C.; Christlieb, N.; François, P.; Hill, V.
2010A&A...522A..26S    Altcode: 2010arXiv1003.4510S
  Context. The primordial nature of the Spite plateau is at odds with
  the WMAP satellite measurements, implying a primordial Li production
  at least three times higher than observed. It has also been suggested
  that A(Li) might exhibit a positive correlation with metallicity below
  [Fe/H] ~ -2.5. Previous samples studied comprised few stars below
  [Fe/H] = -3. <BR /> Aims: We present VLT-UVES Li abundances of 28
  halo dwarf stars between [Fe/H] = -2.5 and -3.5, ten of which have
  [Fe/H] &lt;-3. <BR /> Methods: We determined stellar parameters and
  abundances using four different T<SUB>eff</SUB> scales. The direct
  infrared flux method was applied to infrared photometry. Hα wings were
  fitted with two synthetic grids computed by means of 1D LTE atmosphere
  models, assuming two different self-broadening theories. A grid of Hα
  profiles was finally computed by means of 3D hydrodynamical atmosphere
  models. The Li i doublet at 670.8 nm has been used to measure A(Li)
  by means of 3D hydrodynamical NLTE spectral syntheses. An analytical
  fit of A(Li)<SUB>3D, NLTE</SUB> as a function of equivalent width,
  T<SUB>eff</SUB>, log g, and [Fe/H] has been derived and is made
  available. <BR /> Results: We confirm previous claims that A(Li)
  does not exhibit a plateau below [Fe/H] = -3. We detect a strong
  positive correlation with [Fe/H] that is insensitive to the choice of
  T<SUB>eff</SUB> estimator. From a linear fit, we infer a steep slope
  of about 0.30 dex in A(Li) per dex in [Fe/H], which has a significance
  of 2-3σ. The slopes derived using the four T<SUB>eff</SUB> estimators
  are consistent to within 1σ. A significant slope is also detected
  in the A(Li)-T<SUB>eff</SUB> plane, driven mainly by the coolest
  stars in the sample (T<SUB>eff</SUB> &lt; 6250), which appear to be
  Li-poor. However, when we remove these stars the slope detected in
  the A(Li)-[Fe/H] plane is not altered significantly. When the full
  sample is considered, the scatter in A(Li) increases by a factor
  of 2 towards lower metallicities, while the plateau appears very
  thin above [Fe/H] = -2.8. At this metallicity, the plateau lies at
  &lt;A(Li)<SUB>3D, NLTE</SUB>&gt; = 2.199±0.086. <BR /> Conclusions:
  The meltdown of the Spite plateau below [Fe/H] ~ -3 is established,
  but its cause is unclear. If the primordial A(Li) were that derived
  from standard BBN, it appears difficult to envision a single depletion
  phenomenon producing a thin, metallicity independent plateau above
  [Fe/H] = -2.8, and a highly scattered, metallicity dependent
  distribution below. That no star below [Fe/H] = -3 lies above the
  plateau suggests that they formed at plateau level and experienced
  subsequent depletion. <P />Based on observations made with the ESO Very
  Large Telescope at Paranal Observatory, Chile (Programmes 076.A-0463
  and 077.D-0299).Full Table 3 is 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/522/A26">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/522/A26</A>IDL
  code (appendix) is only available in electronic form at <A
  href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: Diffuse X-rays from PNe with WR-type central stars
Authors: Rühling, U.; Sandin, C.; Steffen, M.; Schönberner, D.;
   Hamann, W. -R.; Todt, H.
2010AIPC.1273..213R    Altcode:
  With the help of detailed nebula modeling and X-ray observations, we
  want to shed light on the enigmatic origin of Wolf-Rayet type central
  stars of planetary nebulae. This method allows us to assign observed
  [WC] stars to one of the proposed evolutionary scenarios, attributing
  the loss of hydrogen to a “late”, “very late”, or an “AGB final”
  thermal pulse (LTP, VLTP and AFTP, respectively). We conclude that
  BD+30° 3639 evolved through an AFTP.

---------------------------------------------------------
Title: The evolution of planetary nebulae. VII. Modelling planetary
    nebulae of distant stellar systems
Authors: Schönberner, D.; Jacob, R.; Sandin, C.; Steffen, M.
2010A&A...523A..86S    Altcode: 2010arXiv1009.0999S
  <BR /> Aims: By means of hydrodynamical models we do the first
  investigations of how the properties of planetary nebulae are affected
  by their metal content and what can be learned from spatially unresolved
  spectrograms of planetary nebulae in distant stellar systems. <BR />
  Methods: We computed a new series of 1D radiation-hydrodynamics
  planetary nebulae model sequences with central stars of 0.595
  M<SUB>⊙</SUB> surrounded by initial envelope structures that differ
  only by their metal content. At selected phases along the evolutionary
  path, the hydrodynamic terms were switched off, allowing the models
  to relax for fixed radial structure and radiation field into their
  equilibrium state with respect to energy and ionisation. The analyses
  of the line spectra emitted from both the dynamical and static models
  enabled us to systematically study the influence of hydrodynamics
  as a function of metallicity and evolution. We also recomputed
  selected sequences already used in previous publications, but now
  with different metal abundances. These sequences were used to study
  the expansion properties of planetary nebulae close to the bright
  cut-off of the planetary nebula luminosity function. <BR /> Results:
  Our simulations show that the metal content strongly influences the
  expansion of planetary nebulae: the lower the metal content, the weaker
  the pressure of the stellar wind bubble, but the faster the expansion of
  the outer shell because of the higher electron temperature. This is in
  variance with the predictions of the interacting-stellar-winds model
  (or its variants) according to which only the central-star wind is
  thought to be responsible for driving the expansion of a planetary
  nebula. Metal-poor objects around slowly evolving central stars
  become very dilute and are prone to depart from thermal equilibrium
  because then adiabatic expansion contributes to gas cooling. We find
  indications that photoheating and line cooling are not fully balanced
  in the evolved planetary nebulae of the Galactic halo. Expansion rates
  based on widths of volume-integrated line profiles computed from our
  radiation-hydrodynamics models compare very well with observations
  of distant stellar system. Objects close to the bright cut-off of the
  planetary nebula luminosity function consist of rather massive central
  stars (&gt;0.6 M<SUB>⊙</SUB>) with optically thick (or nearly thick)
  nebular shells. The half-width-half-maximum velocity during this bright
  phase is virtually independent of metallicity, as observed, but somewhat
  depends on the final AGB-wind parameters. <BR /> Conclusions: The
  observed expansion properties of planetary nebulae in distant stellar
  systems with different metallicities are explained very well by our 1D
  radiation-hydrodynamics models. This result demonstrates convincingly
  that the formation and acceleration of a planetary nebula occurs mainly
  because of ionisation and heating of the circumstellar matter by the
  stellar radiation field, and that the pressure exerted by the shocked
  stellar wind is less important. Determinations of nebular abundances
  by means of photoionisation modelling may become problematic for those
  cases where expansion cooling must be considered.

---------------------------------------------------------
Title: CO5BOLD: COnservative COde for the COmputation of COmpressible
    COnvection in a BOx of L Dimensions with l=2,3
Authors: Freytag, Bernd; Steffen, Matthias; Wedemeyer-Böhm, Sven;
   Ludwig, Hans-Günter; Leenaarts, Jorrit; Schaffenberger, Werner;
   Allard, France; Chiavassa, Andrea; Höfner, Susanne; Kamp, Inga;
   Steiner, Oskar
2010ascl.soft11014F    Altcode:
  CO5BOLD - nickname COBOLD - is the short form of "COnservative
  COde for the COmputation of COmpressible COnvection in a BOx of L
  Dimensions with l=2,3". <P />It is used to model solar and stellar
  surface convection. For solar-type stars only a small fraction of the
  stellar surface layers are included in the computational domain. In
  the case of red supergiants the computational box contains the entire
  star. Recently, the model range has been extended to sub-stellar objects
  (brown dwarfs). <P />CO5BOLD solves the coupled non-linear equations
  of compressible hydrodynamics in an external gravity field together
  with non-local frequency-dependent radiation transport. Operator
  splitting is applied to solve the equations of hydrodynamics (including
  gravity), the radiative energy transfer (with a long-characteristics
  or a short-characteristics ray scheme), and possibly additional 3D
  (turbulent) diffusion in individual sub steps. The 3D hydrodynamics
  step is further simplified with directional splitting (usually). The 1D
  sub steps are performed with a Roe solver, accounting for an external
  gravity field and an arbitrary equation of state from a table. <P
  />The radiation transport is computed with either one of three
  modules: <P />MSrad module: It uses long characteristics. The lateral
  boundaries have to be periodic. Top and bottom can be closed or open
  ("solar module"). <P />LHDrad module: It uses long characteristics
  and is restricted to an equidistant grid and open boundaries at all
  surfaces (old "supergiant module"). <P />SHORTrad module: It uses
  short characteristics and is restricted to an equidistant grid and
  open boundaries at all surfaces (new "supergiant module"). <P />The
  code was supplemented with an (optional) MHD version [Schaffenberger
  et al. (2005)] that can treat magnetic fields. There are also modules
  for the formation and advection of dust available. The current version
  now contains the treatment of chemical reaction networks, mostly used
  for the formation of molecules [Wedemeyer-Böhm et al. (2005)], and
  hydrogen ionization [Leenaarts &amp; Wedemeyer-Böhm (2005)], too. <P
  />CO5BOLD is written in Fortran90. The parallelization is done with
  OpenMP directives.

---------------------------------------------------------
Title: VizieR Online Data Catalog: Fe Abundances in metal-poor stars
    (Sbordone+ 2010)
Authors: Sbordone, L.; Bonifacio, P.; Caffau, E.; Ludwig, H. -G.;
   Behara, N. T.; Gonzalez Hernandez, J. I.; Steffen, M.; Cayrel, R.;
   Freytag, B.; van't Veer, C.; Molaro, P.; Plez, B.; Sivarani, T.; Spite,
   M.; Spite, F.; Beers, T. C.; Christlieb, N.; Francois, P.; Hill, V.
2010yCat..35220026S    Altcode: 2010yCat..35229026S
  Line-by-line abundances for FeI and FeII lines used to estimate
  metallicity and gravity for the program stars. The first column lists
  the star name, then the ion (FeI or FeII) The the wavelength in nm,
  the loggf, the measured EW (pm) and the derived abundance assuming the
  four stellar parameter sets used in the article, respectively 3D, BA,
  ALI and IRFM. <P />(3 data files).

---------------------------------------------------------
Title: The solar photospheric abundance of carbon. Analysis of atomic
    carbon lines with the CO5BOLD solar model
Authors: Caffau, E.; Ludwig, H. -G.; Bonifacio, P.; Faraggiana, R.;
   Steffen, M.; Freytag, B.; Kamp, I.; Ayres, T. R.
2010A&A...514A..92C    Altcode: 2010arXiv1002.2628C
  Context. The analysis of the solar spectra using hydrodynamical
  simulations, with a specific selection of lines, atomic data, and method
  for computing deviations from local thermodynamical equilibrium, has
  led to a downward revision of the solar metallicity, Z. We are using
  the latest simulations computed with the CO5BOLD code to reassess
  the solar chemical composition. Our previous analyses of the key
  elements, oxygen and nitrogen, have not confirmed any extreme downward
  revision of Z, as derived in other works based on hydrodynamical
  models. <BR /> Aims: We determine the solar photospheric carbon
  abundance with a radiation-hydrodynamical CO5BOLD model and compute
  the departures from local thermodynamical equilibrium by using the
  Kiel code. <BR /> Methods: We measured equivalent widths of atomic C
  I lines on high-resolution, high signal-to-noise ratio solar atlases
  of disc-centre intensity and integrated disc flux. These equivalent
  widths were analysed with our latest solar 3D hydrodynamical simulation
  computed with CO5BOLD. Deviations from local thermodynamic equilibrium
  we computed in 1D with the Kiel code, using the average temperature
  structure of the hydrodynamical simulation as a background model. <BR />
  Results: Our recommended value for the solar carbon abundance relies
  on 98 independent measurements of observed lines and is A(C)=8.50
  ± 0.06. The quoted error is the sum of statistical and systematic
  errors. Combined with our recent results for the solar oxygen and
  nitrogen abundances, this implies a solar metallicity of Z = 0.0154
  and Z/X = 0.0211. <BR /> Conclusions: Our analysis implies a solar
  carbon abundance that is about 0.1 dex higher than what was found in
  previous analyses based on different 3D hydrodynamical computations. The
  difference is partly driven by our equivalent width measurements
  (we measure, on average, larger equivalent widths than the other work
  based on a 3D model), in part because of the different properties of
  the hydrodynamical simulations and the spectrum synthesis code. The
  solar metallicity we obtain from the CO5BOLD analyses is in slightly
  better agreement with the constraints of helioseismology than the
  previous 3D abundance results.

---------------------------------------------------------
Title: A 3D-NLTE study of the 670 nm solar lithium feature
Authors: Caffau, Elisabetta; Ludwig, Hans-Günter; Steffen, Matthias;
   Bonifacio, Piercarlo
2010IAUS..268..329C    Altcode:
  We derive the 3D-NLTE lithium abundance in the solar photosphere from
  the Lii line at 670 nm as measured in several solar atlases. The Li
  abundance is obtained from line profile fitting with 1D/3D-LTE/3D-NLTE
  synthetic spectra, considering several possibilities for the
  atomic parameters of the lines blending the Li feature. The 670 nm
  spectral region shows considerable differences in the two available
  disc-centre solar atlases, while the two integrated disc spectra are
  very similar. We obtain A(Li)<SUB>3D-NLTE</SUB> = 1.03. The 1D-LTE
  abundance is 0.07 dex smaller. The line-lists giving the best fit
  for the Sun may fail for other stars, while some line-lists fail to
  reproduce the solar profile satisfactorily. We need a better knowledge
  of the atomic parameters of the lines blending the Li feature in order
  to be able to reproduce both the solar spectrum and the spectra of
  other stars. An improved line-list is also required to derive reliable
  estimates of the isotopic Li ratio in solar-metallicity stars.

---------------------------------------------------------
Title: The role of convection, overshoot, and gravity waves for the
    transport of dust in M dwarf and brown dwarf atmospheres
Authors: Freytag, B.; Allard, F.; Ludwig, H. -G.; Homeier, D.;
   Steffen, M.
2010A&A...513A..19F    Altcode: 2010arXiv1002.3437F
  Context. Observationally, spectra of brown dwarfs indicate the presence
  of dust in their atmospheres while theoretically it is not clear what
  prevents the dust from settling and disappearing from the regions of
  spectrum formation. Consequently, standard models have to rely on ad
  hoc assumptions about the mechanism that keeps dust grains aloft in
  the atmosphere. <BR /> Aims: We apply hydrodynamical simulations to
  develop an improved physical understanding of the mixing properties of
  macroscopic flows in M dwarf and brown dwarf atmospheres, in particular
  of the influence of the underlying convection zone. <BR /> Methods: We
  performed two-dimensional radiation hydrodynamics simulations including
  a description of dust grain formation and transport with the CO5BOLD
  code. The simulations cover the very top of the convection zone and
  the photosphere including the dust layers for a sequence of effective
  temperatures between 900 K and 2800 K, all with log g = 5 assuming solar
  chemical composition. <BR /> Results: Convective overshoot occurs in the
  form of exponentially declining velocities with small scale heights, so
  that it affects only the region immediately above the almost adiabatic
  convective layers. From there on, mixing is provided by gravity waves
  that are strong enough to maintain thin dust clouds in the hotter
  models. With decreasing effective temperature, the amplitudes of the
  waves become smaller but the clouds become thicker and develop internal
  convective flows that are more efficient in transporting and mixing
  material than gravity waves. The presence of clouds often leads to a
  highly structured appearance of the stellar surface on short temporal
  and small spatial scales (presently inaccessible to observations). <BR
  /> Conclusions: We identify convectively excited gravity waves as an
  essential mixing process in M dwarf and brown dwarf atmospheres. Under
  conditions of strong cloud formation, dust convection is the dominant
  self-sustaining mixing component.

---------------------------------------------------------
Title: Convection and <SUP>6</SUP>Li in the atmospheres of metal-poor
    halo stars
Authors: Steffen, Matthias; Cayrel, R.; Bonifacio, P.; Ludwig, H. -G.;
   Caffau, E.
2010IAUS..268..215S    Altcode: 2010arXiv1001.3274S
  Based on 3D hydrodynamical model atmospheres computed with the
  CO<SUP>5</SUP>BOLD code and 3D non-LTE (NLTE) line formation
  calculations, we study the effect of the convection-induced line
  asymmetry on the derived <SUP>6</SUP>Li abundance for a range in
  effective temperature, gravity, and metallicity covering the stars
  of the Asplund et al. (2006) sample. When the asymmetry effect
  is taken into account for this sample of stars, the resulting
  <SUP>6</SUP>Li/<SUP>7</SUP>Li ratios are reduced by about 1.5% on
  average with respect to the isotopic ratios determined by Asplund et
  al. (2006). This purely theoretical correction diminishes the number
  of significant <SUP>6</SUP>Li detections from 9 to 4 (2σ criterion),
  or from 5 to 2 (3σ criterion). In view of this result the existence
  of a <SUP>6</SUP>Li plateau appears questionable. A careful reanalysis
  of individual objects by fitting the observed lithium 6707 Å doublet
  both with 3D NLTE and 1D LTE synthetic line profiles confirms that the
  inferred <SUP>6</SUP>Li abundance is systematically lower when using
  3D NLTE instead of 1D LTE line fitting. Nevertheless, halo stars with
  unquestionable <SUP>6</SUP>Li detection do exist even if analyzed in
  3D-NLTE, the most prominent example being HD 84937.

---------------------------------------------------------
Title: The metal-poor end of the Spite plateau: gravity sensitivity
    of the Hα wings fitting.
Authors: Sbordone, L.; Bonifacio, P.; Caffau, E.; Ludwig, H. -G.;
   Behara, N.; Gonzalez-Hernandez, J. I.; Steffen, M.; Cayrel, R.;
   Freytag, B.; Van't Veer, C.; Molaro, P.; Plez, B.; Sivarani, T.; Spite,
   M.; Spite, F.; Beers, T. C.; Christlieb, N.; François, P.; Hill, V.
2010IAUS..268..355S    Altcode:
  We recently presented (Sbordone et al., 2009a) the largest sample to
  date of lithium abundances in extremely metal-poor (EMP) Halo dwarf and
  Turn-Off (TO) stars. One of the most crucial aspects in estimating Li
  abundances is the T<SUB>eff</SUB> determination, since the Li I 670.8
  nm doublet is highly temperature sensitive. In this short contribution
  we concentrate on the T<SUB>eff</SUB> determination based on Hα wings
  fitting, and on its sensitivity to the chosen stellar gravity.

---------------------------------------------------------
Title: Main-sequence and sub-giant stars in the globular cluster
NGC 6397: The complex evolution of the lithium abundance
Authors: González Hernández, J. I.; Bonifacio, P.; Caffau, E.;
   Steffen, M.; Ludwig, H. -G.; Behara, N.; Sbordone, L.; Cayrel, R.;
   Zaggia, S.
2010IAUS..268..257G    Altcode: 2009arXiv0912.4105G
  Thanks to the high multiplex and efficiency of Giraffe at the VLT
  we have been able for the first time to observe the Li I doublet in
  the Main Sequence stars of a globular cluster. At the same time we
  observed Li in a sample of Sub-Giant stars of the same B-V colour. <P
  />Our final sample is composed of 84 SG stars and 79 MS stars. In
  spite of the fact that SG and MS span the same temperature range we
  find that the equivalent widths of the Li I doublet in SG stars are
  systematically larger than those in MS stars, suggesting a higher Li
  content among SG stars. This is confirmed by our quantitative analysis
  carried out making use of 1D hydrostatic plane-parallel models and
  3D hydrodynamical simulations of the stellar atmospheres. <P />We
  derived the effective temperatures of stars in our the sample from Hα
  fitting. Theoretical profiles were computed using 3D hydrodynamical
  simulations and 1D ATLAS models. Therefore, we are able to determined
  1D and 3D-based effective temperatures. We then infer Li abundances
  taking into account non-local thermodynamical equilibrium effects when
  using both 1D and 3D models. <P />We find that SG stars have a mean
  Li abundance higher by 0.1 dex than MS stars. This result is obtained
  using both 1D and 3D models. We also detect a positive slope of Li
  abundance with effective temperature, the higher the temperature the
  higher the Li abundance, both for SG and MS stars, although the slope
  is slightly steeper for MS stars. These results provide an unambiguous
  evidence that the Li abundance changes with evolutionary status. <P
  />The physical mechanisms responsible for this behaviour are not yet
  clear, and none of the existing models seems to describe accurately
  these observations. Based on these conclusions, we believe that the
  cosmological lithium problem still remains an open question.

---------------------------------------------------------
Title: The evolution of planetary nebulae. VI. On the chemical
    composition of the metal-poor PN G135.9+55.9
Authors: Sandin, C.; Jacob, R.; Schönberner, D.; Steffen, M.; Roth,
   M. M.
2010A&A...512A..18S    Altcode: 2009arXiv0912.5430S
  The actual value of the oxygen abundance of the metal-poor planetary
  nebula <ASTROBJ>PN G135.9+55.9</ASTROBJ> has frequently been debated
  in the literature. We wanted to clarify the situation by making an
  improved abundance determination based on a study that includes both
  new accurate observations and new models. We made observations using
  the method of integral field spectroscopy with the PMAS instrument, and
  also used ultraviolet observations that were measured with HST-STIS. In
  our interpretation of the reduced and calibrated spectrum we used
  for the first time, recent radiation hydrodynamic models, which were
  calculated with several setups of scaled values of mean Galactic disk
  planetary nebula metallicities. For evolved planetary nebulae, such
  as <ASTROBJ>PN G135.9+55.9</ASTROBJ>, it turns out that departures
  from thermal equilibrium can be significant, leading to much lower
  electron temperatures, hence weaker emission in collisionally excited
  lines. Based on our time-dependent hydrodynamic models and the observed
  emission line [O iii] λ5007, we found a very low oxygen content of
  about 1/80 of the mean Galactic disk value. This result is consistent
  with emission line measurements in the ultraviolet wavelength range. The
  C/O and Ne/O ratios are unusually high and similar to those of another
  halo object, BoBn-1. <P />Based in part on observations collected at
  the Centro Astronómico Hispano Alemán (CAHA), operated jointly by the
  Max-Planck-Institut für Astronomie and the Instituto de Astrofísica
  de Andalucia (CSIC).

---------------------------------------------------------
Title: <SUP>6</SUP>Li in metal-poor halo stars: real or spurious?
Authors: Steffen, M.; Cayrel, R.; Bonifacio, P.; Ludwig, H. -G.;
   Caffau, E.
2010IAUS..265...23S    Altcode: 2009arXiv0910.5917S
  The presence of convective motions in the atmospheres of metal-poor
  halo stars leads to systematic asymmetries of the emergent spectral
  line profiles. Since such line asymmetries are very small, they can be
  safely ignored for standard spectroscopic abundance analysis. However,
  when it comes to the determination of the <SUP>6</SUP>Li/<SUP>7</SUP>Li
  isotopic ratio, q(Li)=n(<SUP>6</SUP>Li)/n(<SUP>7</SUP>Li), the
  intrinsic asymmetry of the <SUP>7</SUP>Li line must be taken into
  account, because its signature is essentially indistinguishable from
  the presence of a weak <SUP>6</SUP>Li blend in the red wing of the
  <SUP>7</SUP>Li line. In this contribution we quantity the error of the
  inferred <SUP>6</SUP>Li/<SUP>7</SUP>Li isotopic ratio that arises if
  the convective line asymmetry is ignored in the fitting of the λ6707
  Å lithium blend. Our conclusion is that <SUP>6</SUP>Li/<SUP>7</SUP>Li
  ratios derived by Asplund et al. (2006), using symmetric line profiles,
  must be reduced by typically Δq(Li) ≈ 0.015. This diminishes the
  number of certain <SUP>6</SUP>Li detections from 9 to 4 stars or less,
  casting some doubt on the existence of a <SUP>6</SUP>Li plateau.

---------------------------------------------------------
Title: Solar abundances and 3D model atmospheres
Authors: Ludwig, Hans-Günter; Caffau, Elisabetta; Steffen, Matthias;
   Bonifacio, Piercarlo; Freytag, Bernd; Cayrel, Roger
2010IAUS..265..201L    Altcode: 2009arXiv0911.4248L
  We present solar photospheric abundances for 12 elements from optical
  and near-infrared spectroscopy. The abundance analysis was conducted
  employing 3D hydrodynamical (CO<SUP>5</SUP>BOLD) as well as standard
  1D hydrostatic model atmospheres. We compare our results to others
  with emphasis on discrepancies and still lingering problems, in
  particular exemplified by the pivotal abundance of oxygen. We argue
  that the thermal structure of the lower solar photosphere is very
  well represented by our 3D model. We obtain an excellent match of
  the observed center-to-limb variation of the line-blanketed continuum
  intensity, also at wavelengths shortward of the Balmer jump.

---------------------------------------------------------
Title: The metal-poor end of the Spite plateau
Authors: Sbordone, L.; Bonifacio, P.; Caffau, E.; Ludwig, H. -G.;
   Behara, N.; Gonzalez-Hernandez, J. I.; Steffen, M.; Cayrel, R.;
   Freytag, B.; Van't Veer, C.; Molaro, P.; Plez, B.; Sivarani, T.; Spite,
   M.; Spite, F.; Beers, T. C.; Christlieb, N.; François, P.; Hill, V.
2010IAUS..265...75S    Altcode:
  We present the largest sample available to date of lithium abundances in
  extremely metal poor (EMP) Halo dwarfs. Four T<SUB>eff</SUB> estimators
  are used, including IRFM and Hα wings fitting against 3D hydrodynamical
  synthetic profiles. Lithium abundances are computed by means of 1D and
  3D-hydrodynamical NLTE computations. Below [Fe/H]~-3, a strong positive
  correlation of A(Li) with [Fe/H] appears, not influenced by the choice
  of the Teff estimator. A linear fit finds a slope of about 0.30 dex in
  A(Li) per dex in [Fe/H], significant to 2-3 σ, and consistent within
  1 σ among all the T<SUB>eff</SUB> estimators. The scatter in A(Li)
  increases significantly below [Fe/H]~-3. Above, the plateau lies at
  &lt;A(Li)<SUB>3D, NLTE</SUB>&gt; = 2.199 ± 0.086. If the primordial
  A(Li) is the one derived from standard Big Bang Nucleosynthesis
  (BBN), it appears difficult to envision a single depletion phenomenon
  producing a thin, metallicity independent plateau above [Fe/H] = -2.8,
  and a highly scattered, metallicity dependent distribution below.

---------------------------------------------------------
Title: Accuracy of spectroscopy-based radioactive dating of stars
Authors: Ludwig, H. -G.; Caffau, E.; Steffen, M.; Bonifacio, P.;
   Sbordone, L.
2010A&A...509A..84L    Altcode: 2009arXiv0911.4251L
  Context. Combined spectroscopic abundance analyses of stable and
  radioactive elements can be applied for deriving stellar ages. The
  achievable precision depends on factors related to spectroscopy,
  nucleosynthesis, and chemical evolution. <BR /> Aims: We quantify the
  uncertainties arising from the spectroscopic analysis, and compare these
  to the other error sources. <BR /> Methods: We derive formulae for the
  age uncertainties arising from the spectroscopic abundance analysis,
  and apply them to spectroscopic and nucleosynthetic data compiled
  from the literature for the Sun and metal-poor stars. <BR /> Results:
  We obtained ready-to-use analytic formulae of the age uncertainty for
  the cases of stable+unstable and unstable+unstable chronometer pairs,
  and discuss the optimal relation between to-be-measured age and mean
  lifetime of a radioactive species. Application to the literature
  data indicates that, for a single star, the achievable spectroscopic
  accuracy is limited to about ±20% for the foreseeable future. At
  present, theoretical uncertainties in nucleosynthesis and chemical
  evolution models form the precision bottleneck. For stellar clusters,
  isochrone fitting provides a higher accuracy than radioactive dating,
  but radioactive dating becomes competitive when applied to many cluster
  members simultaneously, reducing the statistical errors by a factor
  √{N}. <BR /> Conclusions: Spectroscopy-based radioactive stellar
  dating would benefit from improvements in the theoretical understanding
  of nucleosynthesis and chemical evolution. Its application to clusters
  can provide strong constraints for nucleosynthetic models.

---------------------------------------------------------
Title: Lithium abundances of main-sequence and subgiant stars in
    the globular cluster NGC 6397
Authors: González Hernández, J. I.; Bonifacio, P.; Caffau, E.;
   Steffen, M.; Ludwig, H. -G.; Behara, N.; Sbordone, L.; Cayrel, R.;
   Zaggia, S.
2010IAUS..266..407G    Altcode: 2009arXiv0910.2305G
  We present FLAMES/GIRAFFE spectroscopy obtained with the Very Large
  Telescope (VLT). Using these observations, we have been able (for the
  first time) to observe the Lii doublet in the main-sequence (MS) stars
  of a globular cluster. We also observed Li in a sample of subgiant (SG)
  stars of the same B - V colour. Our final sample is composed of 84 SG
  and 79 MS stars. In spite of the fact that SG and MS stars span the same
  temperature range, we find that the equivalent widths of the Lii doublet
  in SG stars are systematically greater than in MS stars, suggesting a
  higher Li content among SG stars. This is confirmed by our quantitative
  analysis, which makes use of both 1D and 3D model atmospheres. We find
  that SG stars show, on average, a higher Li abundance, by 0.1 dex, than
  MS stars. We also detect a positive slope of Li abundance with effective
  temperature: the higher the temperature the higher the Li abundance,
  both for SG and MS stars, although the slope is slightly steeper for MS
  stars. These results provide unambiguous evidence that the Li abundance
  changes with evolutionary state. The physical mechanisms that contribute
  to this are not yet clear, since none of the proposed models seem to
  describe accurately the observations. Whether such a mechanism can
  explain the cosmological lithium problem is still an open question.

---------------------------------------------------------
Title: On the Role of Acoustic-Gravity Waves in the Energetics of
    the Solar Atmosphere
Authors: Straus, T.; Fleck, B.; Jefferies, S. M.; McIntosh, S. W.;
   Severino, G.; Steffen, M.; Tarbell, T. D.
2009ASPC..415...95S    Altcode: 2010arXiv1003.3773S
  In a recent paper (Straus et al. 2008) we determined the energy
  flux of internal gravity waves in the lower solar atmosphere using
  a combination of 3D numerical simulations and observations obtained
  with the IBIS instrument operated at the Dunn Solar Telescope and
  the Michelson Doppler Imager (MDI) on SOHO. In this paper we extend
  these studies using coordinated observations from SOT/NFI and SOT/SP
  on Hinode and MDI. The new measurements confirm that gravity waves
  are the dominant phenomenon in the quiet middle/upper photosphere and
  that they transport more mechanical energy than the high-frequency
  (&gt; 5 mHz) acoustic waves, even though we find an acoustic flux 3-5
  times larger than the upper limit estimate of Fossum &amp; Carlsson
  (2006). It therefore appears justified to reconsider the significance of
  (non-M)HD waves for the energy balance of the solar chromosphere.

---------------------------------------------------------
Title: Hydrodynamical simulations of convection-related stellar
    micro-variability. II. The enigmatic granulation background of the
    CoRoT target HD 49933
Authors: Ludwig, H. -G.; Samadi, R.; Steffen, M.; Appourchaux, T.;
   Baudin, F.; Belkacem, K.; Boumier, P.; Goupil, M. -J.; Michel, E.
2009A&A...506..167L    Altcode: 2009arXiv0905.2695L
  Context: Local-box hydrodynamical model atmospheres provide
  statistical information about a star's emergent radiation field
  which allows one to predict the level of its granulation-related
  micro-variability. Space-based photometry is now sufficiently
  accurate to test model predictions. <BR />Aims: We aim to model the
  photometric granulation background of HD 49933 as well as the Sun,
  and compare the predictions to the measurements obtained by the
  &lt;sf&gt;CoRoT&lt;/sf&gt; and &lt;sf&gt;SOHO&lt;/sf&gt; satellite
  missions. <BR />Methods: We construct hydrodynamical model atmospheres
  representing HD 49933 and the Sun, and use a previously developed
  scaling technique to obtain the observable disk-integrated brightness
  fluctuations. We further performed exploratory magneto-hydrodynamical
  simulations to gauge the impact of small scale magnetic fields
  on the synthetic light-curves. <BR />Results: We find that the
  granulation-related brightness fluctuations depend on metallicity. We
  obtain a satisfactory correspondence between prediction and observation
  for the Sun, validating our approach. For HD 49933, we arrive at
  a significant over-estimation by a factor of two to three in total
  power. Locally generated magnetic fields are unlikely to be responsible,
  otherwise existing fields would need to be rather strong to sufficiently
  suppress the granulation signal. Presently suggested updates on the
  fundamental stellar parameters do not improve the correspondence;
  however, an ad-hoc increase of the HD 49933 surface gravity by about
  0.2 dex would eliminate most of the discrepancy. <BR />Conclusions:
  We diagnose a puzzling discrepancy between the predicted and observed
  granulation background in HD 49933, with only rather ad-hoc ideas for
  remedies at hand. <P />The &lt;sf&gt;CoRoT&lt;/sf&gt; space mission,
  launched on December 27th 2006, has been developed and is operated by
  CNES, with the contribution of Austria, Belgium, Brazil, ESA, Germany
  and Spain. CIFIST Marie Curie Excellence Team.

---------------------------------------------------------
Title: Lithium in the globular cluster NGC 6397. Evidence for
    dependence on evolutionary status
Authors: González Hernández, J. I.; Bonifacio, P.; Caffau, E.;
   Steffen, M.; Ludwig, H. -G.; Behara, N. T.; Sbordone, L.; Cayrel,
   R.; Zaggia, S.
2009A&A...505L..13G    Altcode: 2009arXiv0909.0983G
  Context: Most globular clusters are believed to host a single
  stellar population. They can thus be considered a good place to
  study the Spite plateau and to search for possible evolutionary
  modifications of the Li content. <BR />Aims: We want to determine the
  Li content of subgiant (SG) and main sequence (MS) stars of the old,
  metal-poor globular cluster NGC 6397. This work was aimed not only
  at studying possible Li abundance variations but also to investigate
  the cosmological Li discrepancy. <BR />Methods: Here, we present
  FLAMES/GIRAFFE observations of a sample of 84 SG and 79 MS stars in
  NGC 6397 selected in a narrow range of B-V colour and, therefore,
  effective temperatures. We determine both effective temperatures and
  Li abundances using three-dimensional hydrodynamical model atmospheres
  for all the MS and SG stars of the sample. <BR />Results: We find
  a significant difference in the Li abundance between SG stars and
  MS stars, the SG stars having an abundance higher by almost 0.1
  dex on average. We also find a decrease in the lithium abundance
  with decreasing effective temperature, both in MS and SG stars,
  albeit with a significantly different slope for the two classes of
  stars. This suggests that the lithium abundance in these stars is,
  indeed, altered by some process, which is temperature-dependent. <BR
  />Conclusions: The lithium abundance pattern observed in NGC 6397 is
  different from what is found among field stars, casting some doubt on
  the use of globular cluster stars as representative of Population II
  with respect to the lithium abundance. None of the available theories
  of Li depletion appears to satisfactorily describe our observations. <P
  />Based on observations obtained with FLAMES/GIRAFFE at VLT Kueyen
  8.2 m telescope in programme 079.D-0399(A). Table and Figs. 3-10 are
  only available in electronic form at http://www.aanda.org Table 2
  is available in electronic form at http://www.aanda.org and at the
  CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via
  http://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/505/L13

---------------------------------------------------------
Title: The Solar Photospheric Nitrogen Abundance: Determination with
    3D and 1D Model Atmospheres
Authors: Maiorca, E.; Caffau, E.; Bonifacio, P.; Busso, M.; Faraggiana,
   R.; Steffen, M.; Ludwig, H. -G.; Kamp, I.
2009PASA...26..345M    Altcode: 2009arXiv0912.0375M
  We present a new determination of the solar nitrogen abundance
  making use of 3D hydrodynamical modelling of the solar photosphere,
  which is more physically motivated than traditional static 1D
  models. We selected suitable atomic spectral lines, relying on
  equivalent width measurements already existing in the literature. For
  atmospheric modelling we used the co <SUP>5</SUP> bold 3D radiation
  hydrodynamics code. We investigated the influence of both deviations
  from local thermodynamic equilibrium (non-LTE effects) and photospheric
  inhomogeneities (granulation effects) on the resulting abundance. We
  also compared several atlases of solar flux and centre-disc intensity
  presently available. As a result of our analysis, the photospheric
  solar nitrogen abundance is A(N) = 7.86 +/- 0.12.

---------------------------------------------------------
Title: VizieR Online Data Catalog: Lithium in NGC 6397 (Gonzalez
    Hernandez+, 2009)
Authors: Gonzalez Hernandez, J. I.; Bonifacio, P.; Caffau, E.; Steffen,
   M.; Ludwig, H. -G.; Behara, N. T.; Sbordone, L.; Cayrel, R.; Zaggia, S.
2009yCat..35059013G    Altcode:
  Photometric data of the dwarf and subgiant stars of the globular
  cluster NGC 6397. We also provide the signal-to-noise of the spectra,
  the 3D and 1D Halpha-based effective temperatures, 3D Li abundances,
  and the equivalent widths and errors: dEWa: Error of the equivalent
  width measurements estimated from a fitting routine that uses as
  free parameters the velocity shift, the continuum location, and the
  equivalent width of the Li line. dEWb: Error of the equivalent width
  associated to the signal-to-noise ratio and the wavelength dispersion
  of the spectra, derived using Cayrel's formula (Cayrel, 1988, IAU
  Symp. 132: The Impact of Very High S/N Spectroscopy on Stellar Physics,
  132, 345). <P />(1 data file).

---------------------------------------------------------
Title: Impact of granulation effects on the use of Balmer lines as
    temperature indicators
Authors: Ludwig, H. -G.; Behara, N. T.; Steffen, M.; Bonifacio, P.
2009A&A...502L...1L    Altcode: 2009arXiv0906.4697L
  Context: Balmer lines serve as important indicators of stellar
  effective temperatures in late-type stellar spectra. One of their
  modelling uncertainties is the influence of convective flows on
  their shape. <BR />Aims: We aim to characterize the influence of
  convection on the wings of Balmer lines. <BR />Methods: We perform
  a differential comparison of synthetic Balmer line profiles obtained
  from 3D hydrodynamical model atmospheres and 1D hydrostatic standard
  ones. The model parameters are appropriate for F, G, K dwarf and
  subgiant stars of metallicity ranging from solar to 10<SUP>-3</SUP>
  solar. <BR />Results: The shape of the Balmer lines predicted by 3D
  models can never be exactly reproduced by a 1D model, irrespective of
  its effective temperature. We introduce the concept of a 3D temperature
  correction, as the effective temperature difference between a 3D model
  and a 1D model which provides the closest match to the 3D profile. The
  temperature correction is different for the different members of
  the Balmer series and depends on the adopted mixing-length parameter
  α<SUB>MLT</SUB> in the 1D model. Among the investigated models, the
  3D correction ranges from -300 K to +300 K. Horizontal temperature
  fluctuations tend to reduce the 3D correction. <BR />Conclusions:
  Accurate effective temperatures cannot be derived from the wings of
  Balmer lines, unless the effects of convection are properly accounted
  for. The 3D models offer a physically well justified way of doing
  so. The use of 1D models treating convection with the mixing-length
  theory do not appear to be suitable for this purpose. In particular,
  there are indications that it is not possible to determine a single
  value of α<SUB>MLT</SUB> which will optimally reproduce the Balmer
  lines for any choice of atmospheric parameters. The investigation
  of a more extended grid and direct comparison with observed Balmer
  profiles will be carried out in the near future. <P />Appendices is
  only available in electronic form at http://www.aanda.org

---------------------------------------------------------
Title: The solar photospheric nitrogen abundance. Analysis of atomic
    transitions with 3D and 1D model atmospheres
Authors: Caffau, E.; Maiorca, E.; Bonifacio, P.; Faraggiana, R.;
   Steffen, M.; Ludwig, H. -G.; Kamp, I.; Busso, M.
2009A&A...498..877C    Altcode: 2009arXiv0903.3406C
  Context: In recent years, the solar chemical abundances have been
  studied in considerable detail because of discrepant values of
  solar metallicity inferred from different indicators, i.e., on the
  one hand, the “sub-solar” photospheric abundances resulting
  from spectroscopic chemical composition analyses with the aid of
  3D hydrodynamical models of the solar atmosphere, and, on the other
  hand, the high metallicity inferred by helioseismology. <BR />Aims:
  After investigating the solar oxygen abundance using a CO^5BOLD 3D
  hydrodynamical solar model in previous work, we undertake a similar
  approach studying the solar abundance of nitrogen, since this element
  accounts for a significant fraction of the overall solar metallicity,
  Z. <BR />Methods: We used a selection of atomic spectral lines to
  determine the solar nitrogen abundance, relying mainly on equivalent
  width measurements in the literature. We investigate the influence on
  the abundance analysis, of both deviations from local thermodynamic
  equilibrium (“NLTE effects”) and photospheric inhomogeneities
  (“granulation effects”). <BR />Results: We recommend use of a solar
  nitrogen abundance of A(N) = 7.86 ± 0.12, whose error bar reflects
  the line-to-line scatter. <BR />Conclusions: The solar metallicity
  implied by the CO^5BOLD-based nitrogen and oxygen abundances is in the
  range 0.0145≤ Z ≤ 0.0167. This result is a step towards reconciling
  photospheric abundances with helioseismic constraints on Z. Our most
  suitable estimates are Z=0.0156 and Z/X=0.0213.

---------------------------------------------------------
Title: Near-surface stellar magneto-convection: simulations for the
    Sun and a metal-poor solar analog
Authors: Steffen, Matthias; Ludwig, H. -G.; Steiner, O.
2009IAUS..259..233S    Altcode: 2009arXiv0902.2753S
  We present 2D local box simulations of near-surface radiative
  magneto-convection with prescribed magnetic flux, carried out with the
  MHD version of the CO<SUP>5</SUP>BOLD code for the Sun and a solar-like
  star with a metal-poor chemical composition (metal abundances reduced by
  a factor 100, [M/H] = -2). The resulting magneto-hydrodynamical models
  can be used to study the influence of the metallicity on the properties
  of magnetized stellar atmospheres. A preliminary analysis indicates
  that the horizontal magnetic field component tends to be significantly
  stronger in the optically thin layers of metal-poor stellar atmospheres.

---------------------------------------------------------
Title: Convective mixing and dust clouds in the atmospheres of
    brown dwarfs
Authors: Freytag, Bernd; Allard, France; Ludwig, Hans-Günter; Homeier,
   Derek; Steffen, Matthias; Sharp, Christopher
2009AIPC.1094..489F    Altcode: 2009csss...15..489F
  Observed spectra of brown dwarfs demonstrate that their atmospheres
  are influenced by dust. To investigate the mechanism that controls
  the formation and gravitational settling of dust grains as well as the
  mixing of fresh condensable material into the atmosphere, we performed
  2D radiation-hydrodynamics simulations with CO5BOLD. The models comprise
  the upper part of the convection zone and the atmosphere with the
  dust cloud layers. We find that direct convective overshoot does not
  play a major role. Instead, the mixing in the clouds is controlled by
  gravity waves.

---------------------------------------------------------
Title: Effective temperatures of cool metal-poor stars derived from
    the analysis of 3D Balmer lines
Authors: Behara, N. T.; Ludwig, H. -G.; Steffen, M.; Bonifacio, P.
2009AIPC.1094..784B    Altcode: 2009csss...15..784B
  Balmer lines are recognized as accurate indicators of the effective
  temperature of late-type stars. The influence of convection on
  the shape of Balmer line profiles has been investigated using LTE
  3D hydrodynamical model atmospheres and `classical' LTE 1D stellar
  atmospheres, where convection is modeled within the simplistic picture
  of mixing-length theory. Models and line profiles computed with the
  CO<SUP>5</SUP>BOLD and Linfor3D codes have been used to determine
  the effective temperatures of the Sun and three well known metal-poor
  stars HD84937, HD74000, and HD140283. Our 3D fit provides the best fit
  thus far for the solar Hα temperature using the Barklem theory. The
  resulting (3D-1D) Teff biases related to the different treatment of
  convection in the 1D and 3D models are presented.

---------------------------------------------------------
Title: Micro- and macroturbulence derived from 3D hydrodynamical
    stellar atmospheres .
Authors: Steffen, M.; Ludwig, H. -G.; Caffau, E.
2009MmSAI..80..731S    Altcode: 2009arXiv0909.2831S
  The theoretical prediction of micro- and macroturbulence (xi_mic
  and xi_mac ) as a function of stellar parameters can be useful for
  spectroscopic work based on 1D model atmospheres in cases where an
  empirical determination of xi_mic is impossible due to a lack of
  suitable lines and/or macroturbulence and rotational line broadening
  are difficult to separate. In an effort to exploit the CIFIST 3D model
  atmosphere grid for deriving the theoretical dependence of xi_mic and
  xi_mac on effective temperature, gravity, and metallicity, we discuss
  different methods to derive xi_mic from the numerical simulations,
  and report first results for the Sun and Procyon. In both cases the
  preliminary analysis indicates that the microturbulence found in the
  simulations is significantly lower than in the real stellar atmospheres.

---------------------------------------------------------
Title: The CIFIST 3D model atmosphere grid.
Authors: Ludwig, H. -G.; Caffau, E.; Steffen, M.; Freytag, B.;
   Bonifacio, P.; Kučinskas, A.
2009MmSAI..80..711L    Altcode: 2009arXiv0908.4496L
  Grids of stellar atmosphere models and associated synthetic spectra
  are numerical products which have a large impact in astronomy due to
  their ubiquitous application in the interpretation of radiation from
  individual stars and stellar populations. 3D model atmospheres are
  now on the verge of becoming generally available for a wide range
  of stellar atmospheric parameters. We report on efforts to develop
  a grid of 3D model atmospheres for late-type stars within the CIFIST
  Team at Paris Observatory. The substantial demands in computational
  and human labor for the model production and post-processing render
  this apparently mundane task a challenging logistic exercise. At
  the moment the CIFIST grid comprises 77 3D model atmospheres with
  emphasis on dwarfs of solar and sub-solar metallicities. While the
  model production is still ongoing, first applications are already
  worked upon by the CIFIST Team and collaborators.

---------------------------------------------------------
Title: Solar abundances and granulation effects
Authors: Caffau, E.; Ludwig, H. -G.; Steffen, M.
2009MmSAI..80..643C    Altcode: 2009arXiv0910.4733C
  The solar abundances have undergone a major downward revision
  in the last decade, reputedly as a result of employing 3D
  hydrodynamical simulations to model the inhomogeneous structure of
  the solar photosphere. The very low oxygen abundance advocated by
  \citet{asplund04}, A(O)=8.66, together with the downward revision of
  the carbon and nitrogen abundances, has created serious problems for
  solar models to explain the helioseismic measurements. <P />In an
  effort to contribute to the dispute we have re-derived photospheric
  abundances of several elements independently of previous analysis. We
  applied a state-of-the art 3D (CO5BOLD) hydrodynamical simulation
  of the solar granulation as well as different 1D model atmospheres
  for the line by line spectroscopic abundance determinations. The
  analysis is based on both standard disc-centre and disc-integrated
  spectral atlases; for oxygen we acquired in addition spectra at
  different heliocentric angles. The derived abundances are the result
  of equivalent width and/or line profile fitting of the available atomic
  lines. We discuss the different granulation effects on solar abundances
  and compare our results with previous investigations. According to
  our investigations hydrodynamical models are important in the solar
  abundance determination, but are not responsible for the recent downward
  revision in the literature of the solar metallicity.

---------------------------------------------------------
Title: NLTE Abundances of Sodium, Magnesium and Barium in the Globular
    Clusters M10 and M71
Authors: Mishenina, T. V.; Kučinskas, A.; Andrievsky, S. M.; Korotin,
   S. A.; Dobrovolskas, V.; Ivanauskas, A.; Caffau, E.; Ludwig, H. -G.;
   Steffen, M.; Sperauskas, J.; Klochkova, V. G.; Panchuk, V. E.
2009BaltA..18..193M    Altcode: 2009OAst...18..193M
  We derive NLTE abundances of Na, Mg and Ba in four late-type giants
  belonging to globular clusters M10 and M71. The obtained relative
  [Na/Fe] ratios, which were measured only in M10, are positive, with
  the average value [Na/Fe] = +0.3. The ratios [Mg/Fe] in both clusters
  are supersolar, +0.15 to +0.28, while [Ba/Fe] scatter between --0.14
  and +0.09. Differences between the NLTE abundances derived in this
  work and those obtained in LTE by Mishenina et al. (2003) are small,
  typically within ±0.1 dex. We also perform numerical simulations with
  the CO<SUP>5</SUP>BOLD 3D hydrodynamical stellar atmosphere code to
  investigate the influence of convection on the formation of spectral
  lines used in our NLTE study. For this purpose we use a model of
  late-type giant with T<SUB></SUB> eff = 4020 K, log g = 1.0, [M/H] =
  --1.0 and find that for Na, Mg and Ba the 3D--1D abundance corrections
  are below ∼ 0.02 dex. However, their size strongly depends on the
  value of microturbulent velocity used with the 1D model.

---------------------------------------------------------
Title: Simulations of dust clouds in the atmospheres of substellar
    objects.  Theory toddles after observations
Authors: Freytag, B.; Allard, F.; Ludwig, H. -G.; Homeier, D.;
   Steffen, M.
2009MmSAI..80..670F    Altcode:
  The atmospheres of brown dwarfs allow the formation of dust grains
  and their rain-out into deeper, invisible layers. However, observed
  spectra of L dwarfs can only be reproduced when static 1D models
  account for dust formation and its resulting greenhouse effect in the
  visible layers. Time-dependent hydrodynamical processes can mix up the
  material giving rise to complex unsteady weather phenomena on these
  objects. We performed radiation hydrodynamics simulations in two and
  three dimensions of the atmospheres of brown dwarfs with CO5BOLD,
  including a treatment of dust particles. We find that exponential
  overshoot (close to the gas convection zone), gravity waves (weak
  omni-present mixing), and convection within dust layers (in the thick
  clouds in cooler models) contribute to the atmospheric mixing, which
  is far from being a stationary process. The presence of dust in the
  atmospheres is accompanied by large temporal and spatial intensity
  fluctuations.

---------------------------------------------------------
Title: 3D hydrodynamical simulations of stellar photospheres with
    the CO<SUP>5</SUP>BOLD code. Photometric colors of a late-type giant
Authors: Kučinskas, A.; Ludwig, H. -G.; Caffau, E.; Steffen, M.
2009MmSAI..80..723K    Altcode: 2009arXiv0910.3412K
  We present synthetic broad-band photometric colors of a late-type
  giant located close to the RGB tip (T_eff≈3640 K, log g=1.0 and
  [M/H]=0.0). Johnson-Cousins-Glass BVRIJHK colors were obtained from
  the spectral energy distributions calculated using 3D hydrodynamical
  and 1D classical stellar atmosphere models. The differences between
  photometric magnitudes and colors predicted by the two types of models
  are significant, especially at optical wavelengths where they may
  reach, e.g., Delta V≈0.16, Delta R≈0.13 and Delta (V-I)≈0.14,
  Delta (V-K)≈0.20. Differences in the near-infrared are smaller but
  still non-negligible (e.g., Delta K≈ 0.04). Such discrepancies may
  lead to noticeably different photometric parameters when these are
  inferred from photometry (e.g., effective temperature will change by
  Delta T_eff≈60 K due to difference of Delta (V-K)≈0.20).

---------------------------------------------------------
Title: Solar Photosphere and Chromosphere
Authors: Steffen, Matthias
2009LanB...4B...28S    Altcode: 2009LanB...4B.4114S
  No abstract at ADS

---------------------------------------------------------
Title: Monitoring mass motions of Betelgeuse's photosphere using
    robotic telescopes .
Authors: Weber, M.; Carroll, T.; Granzer, T.; Steffen, M.; Strassmeier,
   K. G.
2009MmSAI..80..743W    Altcode:
  We started monitoring Betelgeuse using STELLA/SES, the STELLA
  échelle spectrograph fed by a robotic 1.2 m telescope on Tenerife,
  and the automatic photometric telescope (APT) T7 in Arizona in fall
  2008. In this first observing season, we have collected 67 high
  resolution spectra from 390 to 900 nm at a resolution of 50,000 and
  a S/N between 100 and 300, and a comparable number of photometric
  observations in the Halpha filter. In this presentation, we report on
  the initial findings based on this first data set: Radial velocities,
  effective temperature (along with surface gravity and metallicity) are
  automatically computed by the STELLA/SES data reduction &amp; analysis
  pipeline. We compare these global measurements and the photometric
  brightness with velocities and temperature indicators derived from
  individual spectral lines, to bring these values in line with recently
  published observations. Furthermore we compute synthetic line profiles
  from state-of-the-art 3D stellar convection models, and compare the
  line-profiles, their shapes and positions to our observations. The
  final aim of the observing program is to find out if the spectral line
  variations can be explained using these non-magnetic convection models.

---------------------------------------------------------
Title: Models of surface convection and dust clouds in brown dwarfs
Authors: Freytag, B.; Allard, F.; Ludwig, H. -G.; Homeier, D.;
   Steffen, M.
2008PhST..133a4005F    Altcode:
  The influence of dust grains on the atmospheres of brown dwarfs is
  visible in observed spectra. To investigate what prevents the dust
  grains from falling down, or how fresh condensable material is mixed
  up in the atmosphere to allow new grains to form, we performed 2D
  radiation-hydrodynamics simulations with CO5BOLD of the upper part
  of the convection zone and the atmosphere containing the dust cloud
  layers. We find that unlike in models of Cepheids, the convective
  overshoot does not play a major role. Instead, the mixing in the dust
  clouds is controlled by gravity waves.

---------------------------------------------------------
Title: he models comprise the upper part of the convection zone
    and the atmosphere with %the dust cloud layers. We find that direct
    convective overshoot does not play a major role. Instead, the mixing
    in the clouds is controlled by gravity waves.
Authors: Freytag, B.; Allard, F.; Ludwig, H. -G.; Homeier, D.; Steffen,
   M.; Sharp, C.
2008sf2a.conf..469F    Altcode:
  To investigate the mechanism that controls the formation and
  gravitational settling of dust grains as well as the mixing of fresh
  condensable material into the atmosphere of brown dwarfs, we performed
  2D radiation-hydrodynamics simulations with CO5BOLD.

---------------------------------------------------------
Title: The evolution of planetary nebulae. V. The diffuse X-ray
    emission
Authors: Steffen, M.; Schönberner, D.; Warmuth, A.
2008A&A...489..173S    Altcode: 2008arXiv0807.3290S
  Context: Observations with space-borne X-ray telescopes revealed the
  existence of soft, diffuse X-ray emission from the inner regions of
  planetary nebulae. Although the existing images support the idea that
  this emission arises from the hot shocked central-star wind which
  fills the inner cavity of a planetary nebula, existing models have
  difficulties to explain the observations consistently. <BR />Aims: We
  investigate how the inclusion of thermal conduction changes the physical
  parameters of the hot shocked wind gas and the amount of X-ray emission
  predicted by time-dependent hydrodynamical models of planetary nebulae
  with central stars of normal, hydrogen-rich surface composition. <BR
  />Methods: We upgraded our 1D hydrodynamics code NEBEL by to account
  for energy transfer due to heat conduction, which is of importance at
  the interface separating the hot shocked wind gas (“hot bubble”)
  from the much cooler nebular material. With this new version of
  NEBEL we recomputed a selection of our already existing hydrodynamical
  sequences and obtained synthetic X-ray spectra for representative models
  along the evolutionary tracks by means of the freely available CHIANTI
  package. <BR />Results: Heat conduction leads to lower temperatures and
  higher densities within a bubble and brings the physical properties
  of the X-ray emitting domain into close agreement with the values
  derived from observations. The amount of X-rays emitted during the
  course of evolution depends on the energy dumped into the bubble by
  the fast stellar wind, on the efficiency of “evaporating” cool
  nebular gas via heat conduction, and on the bubble's expansion rate. We
  find from our models that the X-ray luminosity of a planetary nebula
  increases during its evolution across the HR diagram until stellar
  luminosity and wind power decline. Depending on the central-star mass
  and the evolutionary phase, our models predict X-ray [ 0.45-2.5
  keV] luminosities between 10<SUP>-8</SUP> and 10<SUP>-4</SUP>
  of the stellar bolometric luminosities, in good agreement with the
  observations. Less than 1% of the wind power is radiated away in this
  X-ray band. Although temperature, density, and also the mass of the
  hot bubble is significantly altered by heat conduction, the dynamics
  of the whole system remains practically the same. <BR />Conclusions:
  Heat conduction allows the construction of nebular models which predict
  the correct amount of X-ray emission and at the same time are fully
  consistent with the observed mass-loss rate and wind speed. Thermal
  conduction must be considered as a viable physical process for
  explaining the diffuse X-ray emission from planetary nebulae with
  closed inner cavities. Magnetic fields must then be absent or extremely
  weak. <P />Dedicated to the memory of M. Perinotto, a dear friend and
  esteemed colleague who died unexpectedly and much too <P />early on
  August 15, 2007.

---------------------------------------------------------
Title: On the Role of Acoustic-gravity Waves in the Energetics of
    the Solar Atmosphere
Authors: Straus, T.; Fleck, B.; Jefferies, S. M.; Cauzzi, G.; McIntosh,
   S. W.; Reardon, K.; Severino, G.; Steffen, M.; Suter, M.; Tarbell,
   T. D.
2008ESPM...12.2.11S    Altcode:
  We revisit the dynamics and energetics of the solar atmosphere, using a
  combination of high-quality observations and 3D numerical simulations
  of the overshoot region of compressible convection into the stable
  photosphere. We discuss the contribution of acoustic-gravity waves
  to the energy balance of the photosphere and low chromosphere. We
  demonstrate the presence of propagating internal gravity waves at
  low frequencies (&lt; 5mHz). Surprisingly, these waves are found
  to be the dominant phenomenon in the quiet middle/upper photosphere
  and to transport a significant amount of mechanical energy into the
  atmosphere outweighing the contribution of high-frequency (&gt; 5mHz)
  acoustic waves by more than an order of magnitude. We compare the
  properties of high-frequency waves in the simulations with results
  of recent high cadence, high resolution Doppler velocity measurements
  obtained with SOT/SP and SOT/NFI on Hinode. Our results seem to be in
  conflict with the simple picture of upward propagating sound waves. We
  discuss the implications of our findings on the energy flux estimate
  at high-frequencies.

---------------------------------------------------------
Title: The Solar Photospheric Oxygen Abundance and the Role of 3D
    Model Atmospheres
Authors: Caffau, E.; Steffen, M.; Ludwig, H. -G.
2008ESPM...12..3.7C    Altcode:
  The solar oxygen abundance has undergone a major downward revision in
  the last decade, reputedly as a result of employing 3D hydrodynamical
  simulations to model the inhomogeneous structure of the solar
  photosphere. <P />The very low oxygen abundance advocated by Asplund
  et al. 2004, A(O)=8.66, together with the downward revision of the
  abundances of other key elements, has created serious problems for solar
  models to explain the helioseismic measurements. <P />In an effort to
  contribute to the dispute of whether the Sun has "solar" or "sub-solar"
  abundances, we have re-derived its photospheric abundance of oxygen,
  nitrogen, and other elements, independently of previous analyses. <P
  />We applied a state-of-the art 3D (CO5BOLD) hydrodynamical simulation
  of the solar granulation as well as different 1D model atmospheres for
  the line by line spectroscopic abundance determinations. The analysis
  is based on both standard disk-center and full-disk spectral atlases;
  for oxygen we acquired in addition spectra at different heliocentric
  angles. The derived abundances are the result of equivalent width
  and/or line profile fitting of the available atomic lines. Our
  recommended oxygen abundance is A(O)=8.76+- 0.07, 0.1 dex higher
  than the value of Asplund et al. (2004). Our current estimate of the
  overall solar metallicity is 0.014&lt; Z&lt;0.016. <P />Questions we
  discuss include: (i) Is the general downward revision of the solar
  abundances a 3D effect? (ii) How large are the abundance corrections
  due to horizontal inhomogeneities? (iii) What is the main reason for
  the differences between the abundances obtained in our study and those
  derived by Apslund and coworkers? (iv) How large are the uncertainties
  in the observed solar spectra? (v) What is the reason why the two
  forbidden oxygen lines, [OI] lambda 630 nm and [OI] lambda 636.3 nm,
  give significantly different answers for the solar oxygen abundance?

---------------------------------------------------------
Title: The photospheric solar oxygen project. I. Abundance analysis
    of atomic lines and influence of atmospheric models
Authors: Caffau, E.; Ludwig, H. -G.; Steffen, M.; Ayres, T. R.;
   Bonifacio, P.; Cayrel, R.; Freytag, B.; Plez, B.
2008A&A...488.1031C    Altcode: 2008arXiv0805.4398C
  Context: The solar oxygen abundance has undergone a major downward
  revision in the past decade, the most noticeable one being the
  update including 3D hydrodynamical simulations to model the solar
  photosphere. Up to now, such an analysis has only been carried out
  by one group using one radiation-hydrodynamics code. <BR />Aims:
  We investigate the photospheric oxygen abundance considering lines
  from atomic transitions. We also consider the relationship between
  the solar model used and the resulting solar oxygen abundance, to
  understand whether the downward abundance revision is specifically
  related to 3D hydrodynamical effects. <BR />Methods: We performed
  a new determination of the solar photospheric oxygen abundance by
  analysing different high-resolution high signal-to-noise ratio atlases
  of the solar flux and disc-centre intensity, making use of the latest
  generation of CO5BOLD 3D solar model atmospheres. <BR />Results: We
  find 8.73 ≤ log (N_O/N_H) +12 ≤ 8.79. The lower and upper values
  represent extreme assumptions on the role of collisional excitation
  and ionisation by neutral hydrogen for the NLTE level populations
  of neutral oxygen. The error of our analysis is ± (0.04± 0.03)
  dex, the last being related to NLTE corrections, the first error
  to any other effect. The 3D “granulation effects” do not play a
  decisive role in lowering the oxygen abundance. <BR />Conclusions:
  Our recommended value is log (N_O/N_H) = 8.76 ± 0.07, considering our
  present ignorance of the role of collisions with hydrogen atoms on the
  NLTE level populations of oxygen. The reasons for lower O abundances in
  the past are identified as (1) the lower equivalent widths adopted and
  (2) the choice of neglecting collisions with hydrogen atoms in the
  statistical equilibrium calculations for oxygen. <P />This paper is
  dedicated to the memory of Hartmut Holweger.

---------------------------------------------------------
Title: Velocity and Intensity Power and Cross Spectra in Numerical
    Simulations of Solar Convection
Authors: Severino, G.; Straus, T.; Steffen, M.
2008SoPh..251..549S    Altcode: 2008SoPh..tmp...54S
  Fitting observed power and cross spectra of medium-degree p modes
  in velocity (V) and intensity (I) has been widely used for getting
  information about the p-mode excitation process and, in particular,
  for trying to determine the type and location of the acoustic
  sources. Numerical simulations of solar convection allow one to
  "observe" velocity and temperature (T, used as proxy for I) fluctuations
  in different reference frames. Sampling the oscillations on planes of
  constant optical depth (τ-frame) closely corresponds to the observer's
  point of view, whereas sampling the oscillations at constant geometrical
  height (z-frame) is more appropriate for comparison with predictions
  from theoretical models based on Eulerian hydrodynamics. The results of
  the analysis in the two frames show significant differences. Considering
  the effects introduced on oscillations by the steep temperature gradient
  of the photosphere and by the temperature- and pressure-dependent
  continuum opacity, we develop a new model for fitting the simulated V
  and T power and cross spectra both in the τ- and z-frames and discuss
  its merits and limitations.

---------------------------------------------------------
Title: Radiation hydrodynamics simulations of stellar surface
    convection
Authors: Freytag, Bernd; Steffen, Matthias; Ludwig, Hans-Guenter;
   Wedemeyer-Boehm, Sven
2008asd..soft...36F    Altcode:
  The code is used to perform radiation hydrodynamics simulations of
  the convective surface layers and the photosphere of cool stars.

---------------------------------------------------------
Title: Spatially resolved spectroscopy of planetary nebulae and
    their halos. I. Five galactic disk objects
Authors: Sandin, C.; Schönberner, D.; Roth, M. M.; Steffen, M.;
   Böhm, P.; Monreal-Ibero, A.
2008A&A...486..545S    Altcode: 2008arXiv0802.3813S
  Strong mass loss off stars at the tip of the asymptotic giant
  branch (AGB) profoundly affects properties of these stars and their
  surroundings, including the subsequent planetary nebula (PN) stage. With
  this study we wanted to determine physical properties of mass loss by
  studying weakly emitting halos, focusing on objects in the galactic
  disk. Halos surround the, up to several thousand times, brighter
  central regions of PNe. Young halos, specifically, still contain
  information of the preceeding final mass loss stage on the AGB. In
  the observations we used the method of integral field spectroscopy
  with the PMAS instrument. This is the first committed study of halos
  of PNe that uses this technique. We improved our data analysis by a
  number of steps. In a study of the influence of scattered light we found
  that a moderate fraction of intensities in the inner halo originate in
  adjacent regions. As we combine line intensities of distant wavelengths,
  and because radial intensity gradients are steep, we corrected for
  effects of differential atmospheric refraction. In order to increase
  the signal-to-noise of weak emission lines we introduced a dedicated
  method to bin spectra of individual spatial elements. We also developed
  a general technique to part the temperature-sensitive oxygen line [O
  III] λ4363 from the adjacent telluric mercury line Hg λ4358 - without
  using separate sky exposures. By these steps we avoided introducing
  errors of several thousand Kelvin to our temperature measurements in the
  halo. For IC 3568 we detected a halo. For M 2-2 we found a halo radius
  that is 2.5 times larger than reported earlier. We derived radially
  densely sampled temperature and density structures for four nebulae,
  which all extend from the central regions and out into the halo. NGC
  7662, IC 3568, and NGC 6826 show steep radially increasing temperatures
  and a hot halo, indicating that the gas in the halo is not in thermal
  equilibrium. M 2-2 shows a larger temperature in the central region
  and an otherwise constant value. From the density structures we made
  estimates of core and halo masses and - for the first time reliable -
  mass loss rates at the tip of the AGB. All four objects show inwards
  radially increasing mass loss rate structures, which represent a rise
  by a factor of about 4-7, during the final mass loss phase, that covers
  a time period of approximately 10<SUP>4</SUP> years. Within a factor
  of two, the average of the maximum mass loss rates, which are distance
  dependent, is dot{M}<SUB>max</SUB>≃10<SUP>-4</SUP> {M}<SUB>⊙</SUB>
  yr<SUP>-1</SUP>. <P />Based on observations collected at the Centro
  Astronómico Hispano Alemán (CAHA), operated jointly by the Max-Planck
  Institut für Astronomie and the Instituto de Astrofísica de Andalucia
  (CSIC). <P />Figures 24-29 are only available in electronic form at
  http://www.aanda.org

---------------------------------------------------------
Title: The Energy Flux of Internal Gravity Waves in the Lower Solar
    Atmosphere
Authors: Straus, Thomas; Fleck, Bernhard; Jefferies, Stuart M.;
   Cauzzi, Gianna; McIntosh, Scott W.; Reardon, Kevin; Severino, Giuseppe;
   Steffen, Matthias
2008ApJ...681L.125S    Altcode:
  Stably stratified fluids, such as stellar and planetary atmospheres,
  can support and propagate gravity waves. On Earth these waves,
  which can transport energy and momentum over large distances and can
  trigger convection, contribute to the formation of our weather and
  global climate. Gravity waves also play a pivotal role in planetary
  sciences and modern stellar physics. They have also been proposed
  as an agent for the heating of stellar atmospheres and coronae, the
  exact mechanism behind which is one of the outstanding puzzles in solar
  and stellar physics. Using a combination of high-quality observations
  and 3D numerical simulations we have the first unambiguous detection
  of propagating gravity waves in the Sun's (and hence a stellar)
  atmosphere. Moreover, we are able to determine the height dependence of
  their energy flux and find that at the base of the Sun's chromosphere it
  is around 5 kW m<SUP>-2</SUP>. This amount of energy is comparable to
  the radiative losses of the entire chromosphere and points to internal
  gravity waves as a key mediator of energy into the solar atmosphere.

---------------------------------------------------------
Title: Toward Better Simulations of Planetary Nebulae Luminosity
    Functions
Authors: Méndez, R. H.; Teodorescu, A. M.; Schönberner, D.; Jacob,
   R.; Steffen, M.
2008ApJ...681..325M    Altcode: 2008arXiv0804.0826M
  We describe a procedure for the numerical simulation of the planetary
  nebulae luminosity function (PNLF), improving on previous work. Earlier
  PNLF simulations were based on an imitation of the observed distribution
  of the intensities of [O III] λ5007 relative to Hβ, generated
  predominantly using random numbers. We are now able to replace this
  by a distribution derived from the predictions of hydrodynamical
  PN models (Schönberner et al. 2007), which are made to evolve as
  the central star moves across the HR diagram, using proper initial
  and boundary conditions. In this way we move one step closer to a
  physically consistent procedure for the generation of a PNLF. As an
  example of these new simulations, we have been able to reproduce the
  observed PNLF in the Small Magellanic Cloud.

---------------------------------------------------------
Title: The solar photospheric abundance of hafnium and
    thorium. Results from CO<SUP>5</SUP>BOLD 3D hydrodynamic model
    atmospheres
Authors: Caffau, E.; Sbordone, L.; Ludwig, H. -G.; Bonifacio, P.;
   Steffen, M.; Behara, N. T.
2008A&A...483..591C    Altcode: 2008arXiv0803.3585C
  Context: The stable element hafnium (Hf) and the radioactive element
  thorium (Th) were recently suggested as a suitable pair for radioactive
  dating of stars. The applicability of this elemental pair needs to
  be established for stellar spectroscopy. <BR />Aims: We aim at a
  spectroscopic determination of the abundance of Hf and Th in the
  solar photosphere based on a CO<SUP>5</SUP>BOLD 3D hydrodynamical
  model atmosphere. We put this into a wider context by investigating 3D
  abundance corrections for a set of G- and F-type dwarfs. <BR />Methods:
  High-resolution, high signal-to-noise solar spectra were compared to
  line synthesis calculations performed on a solar CO<SUP>5</SUP>BOLD
  model. For the other atmospheres, we compared synthetic spectra
  of CO<SUP>5</SUP>BOLD 3D and associated 1D models. <BR />Results:
  For Hf we find a photospheric abundance A(Hf) = 0.87 ± 0.04, in good
  agreement with a previous analysis, based on 1D model atmospheres. The
  weak Th II 401.9 nm line constitutes the only Th abundance indicator
  available in the solar spectrum. It lies in the red wing of a Ni-Fe
  blend exhibiting a non-negligible convective asymmetry. Accounting for
  the asymmetry-related additional absorption, we obtain A(Th) = 0.08 ±
  0.03, consistent with the meteoritic abundance, and about 0.1 dex lower
  than obtained in previous photospheric abundance determinations. <BR
  />Conclusions: Only for the second time, to our knowledge, has a
  non-negligible effect of convective line asymmetries on an abundance
  derivation been highlighted. Three-dimensional hydrodynamical
  simulations should be employed to measure Th abundances in dwarfs
  if similar blending is present, as in the solar case. In contrast,
  3D effects on Hf abundances are small in G- to mid F-type dwarfs and
  sub-giants, and 1D model atmospheres can be conveniently used.

---------------------------------------------------------
Title: Hydrodynamical Model Atmospheres of Metal-Poor Stars
Authors: Ludwig, Hans-Günter; González Hernández, Jonay I.; Behara,
   Natalie; Caffau, Elisabetta; Steffen, Matthias
2008AIPC..990..268L    Altcode:
  Standard one-dimensional (1D) model atmospheres rely on the assumption
  of radiative equilibrium in the non-convective part of the stellar
  photosphere. However, gas-dynamical effects can lead to dramatic
  deviations from radiative equilibrium conditions, especially in
  metal-poor stellar atmospheres. These can be taken into account in
  3D stellar atmosphere models representing the detailed interplay of
  hydrodynamics and radiation. During the last two years efforts have been
  invested to compute such 3D models for metal-poor atmospheres with the
  CO<SUP>5</SUP> BOLD code within the CIFIST (Cosmological Impact of the
  FIrst STars) Team, an European Union funded research group dedicated
  to the study of metal-poor stars. Based on the available models we will
  give an account of the radiation-hydrodynamical processes at work, and
  discuss consequences for the temperature scale and abundance analysis
  of metal-poor stars.

---------------------------------------------------------
Title: Hydrodynamical Model Atmospheres and 3D Spectral Synthesis
Authors: Ludwig, Hans-Günter; Steffen, Matthias
2008psa..conf..133L    Altcode: 2007arXiv0704.1176L
  In this paper we discuss three issues in the context of
  three-dimensional (3D) hydrodynamical model atmospheres for late-type
  stars, related to spectral line shifts, radiative transfer in metal-poor
  3D models, and the solar oxygen abundance. To establish the context we
  start by giving a brief overview about the model construction, taking
  the radiation-hydrodynamics code CO<SUP>5</SUP>BOLD (Conservative COde
  for the Computation of COmpressible COnvection in a BOx of L Dimensions
  with L=2,3; [3]) and the related spectral synthesis package Linfor3D
  as examples.

---------------------------------------------------------
Title: Overview of the Li problem in metal-poor stars and new results
    on 6Li
Authors: Cayrel, R.; Steffen, M.; Bonifacio, P.; Ludwig, H. -G.;
   Caffau, E.
2008nuco.confE...2C    Altcode: 2008arXiv0810.4290C; 2008PoS....53E...2C
  Two problems are discussed here. The first one is the 0.4 dex
  discrepancy between the 7Li abundance derived from the spectra
  of metal-poor halo stars on the one hand, and from Big Bang
  nucleosynthesis, based on the cosmological parameters constrained
  by the WMAP measurements, on the other hand. Lithium, indeed,
  can be depleted in the convection zone of unevolved stars. The
  understanding of the hydrodynamics of the crucial zone near the
  bottom of the convective envelope in dwarfs or turn-off stars of solar
  metallicity has recently made enormous progress with the inclusion of
  internal gravity waves. However, similar work for metal-poor stars is
  still lacking. Therefore it is not yet clear whether the depletion
  occurring in the metal-poor stars themselves is adequate to produce
  a 7Li plateau. The second problem pertains to the large amount of
  6Li recently found in metal-poor halo stars. The convection-related
  asymmetry of the 7Li line could mimic the signal attributed so far
  to the weak blend of 6Li in the red wing of the 7Li line. Theoretical
  computations show that the signal generated by the asymmetry of 7Li is
  2.0, 2.1, and 3.7 per cent for [Fe/H]= -3.0, -2.0, -1.0, respectively
  (Teff =6250 K and log g=4.0 [cgs]). In addition we re-investigate
  the statistical properties of the 6Li plateau and show that previous
  analyses were biased. Our conclusion is that the 6Li plateau can be
  reinterpreted in terms of intrinsic line asymmetry, without the need
  to invoke a contribution of 6Li. (abridged)

---------------------------------------------------------
Title: Rotating `star-in-a-box' experiments
Authors: Steffen, M.; Freytag, B.
2007AN....328.1054S    Altcode:
  Using the radiation hydrodynamics code CO<SUP>5</SUP>BOLD in its
  `star-in-a-box' setup, we have performed exploratory simulations
  of global convection in a rotating reference frame. The goal is to
  study the interaction of convection and rotation by direct numerical
  simulation. For these first experiments, we chose an idealized
  configuration (a scaled-down, fast rotating Sun) whose properties
  resemble those of red supergiants in some respect. We describe the setup
  and time evolution of these models, and discuss the particular problems
  we have encountered. Finally, we derive the resulting differential
  rotation pattern and meridional flow field by temporal and azimuthal
  averaging of the simulation data. We find anti-solar differential
  rotation for all cases studied so far. <P />Movies are available via
  http://www.aip.de/AN/movies

---------------------------------------------------------
Title: On the Mass-Loss History at the Tip of the AGB
Authors: Schönberner, D.; Steffen, M.
2007ASPC..378..343S    Altcode:
  We demonstrate by means of radiation-hydrodynamics simulations how the
  spectral energy distribution (SED) of post-AGB objects depends on the
  mass-loss properties during evolution off the tip of the AGB.

---------------------------------------------------------
Title: A hydrodynamical study of multiple-shell planetary
    nebulae. II. Measuring the post-shock velocities in the shells
Authors: Corradi, R. L. M.; Steffen, M.; Schönberner, D.; Jacob, R.
2007A&A...474..529C    Altcode:
  Context: Planetary Nebulae (PNe) display complex radial surface
  brightness profiles whose understanding is crucial for a correct
  interpretation of their formation and evolution. In particular, the
  intermediate shells commonly observed around the bright rims of PNe
  contain important information for the discussion of the mass loss rate
  at the end of the AGB, for the determination of the post-AGB age of
  the central stars and the distance via the expansion parallax method,
  and for the analysis of line profiles for unresolved, faraway objects
  like extragalactic PNe. <BR />Aims: This paper describes the dynamical
  properties of PNe shells and presents a new practical method to properly
  determine their expansion velocity. <BR />Methods: The analysis is
  guided by realistic radiative-hydrodynamical simulations which allow
  to test and verify different methods for the kinematical study of
  PNe shells using high-resolution long-slit spectra. <BR />Results: We
  show that the use of the derivative of the line profile allows us to
  determine accurately the post-shock gas velocity in the shells. This
  method is generally superior to other techniques previously used. In
  addition, if applied to long-slit data, it allows to determine the
  velocities of the shells even when they are very close to those of the
  PNe rims. Its application to 10 real PNe confirms the model predictions
  and previous conclusions about the substantial mass loss increase
  during the latest AGB evolution. <BR />Conclusions: The method and
  discussion presented in this paper are meant to be used as a guide
  for a correct determination of some basic kinematic and evolutionary
  properties of Galactic and extragalactic PNe, including their expansion
  parallaxes. <P />Based on observations obtained at the 3.5 m NTT and
  CAT telescopes of the European Southern Observatory in Chile, and at
  the 2.6 m NOT telescope operated by NOTSA in the Spanish Observatorio
  del Roque de Los Muchachos of the Instituto de Astrofísica de Canarias.

---------------------------------------------------------
Title: The solar photospheric abundance of phosphorus: results from
    CO^5BOLD 3D model atmospheres
Authors: Caffau, E.; Steffen, M.; Sbordone, L.; Ludwig, H. -G.;
   Bonifacio, P.
2007A&A...473L...9C    Altcode: 2007arXiv0708.1607C
  Aims:We determine the solar abundance of phosphorus using CO^5BOLD
  3D hydrodynamic model atmospheres. <BR />Methods: High-resolution,
  high signal-to-noise solar spectra of the P i lines of Multiplet 1 at
  1051-1068 nm are compared to line-formation computations performed
  on a CO^5BOLD solar model atmosphere. <BR />Results: We find A(P)
  = 5.46 ± 0.04, in good agreement with previous analyses based on
  1D model atmospheres, due to the P i lines of Mult. 1 not being
  affected much by 3D effects. We cannot confirm an earlier claim by
  other authors of a downward revision of the solar P abundance by 0.1
  dex when employing a 3D model atmosphere. Concerning other stars,
  we find modest (&lt;0.1 dex) 3D abundance corrections for P among
  four F-dwarf model atmospheres of different metallicities, and these
  corrections are largest at lowest metallicity. <BR />Conclusions:
  We conclude that 3D abundance corrections are generally rather small
  for the P i lines studied in this work. They are marginally relevant
  for metal-poor stars, but may be neglected in the Sun. <P />Tables
  2-4 are only available in electronic form at http://www.aanda.org

---------------------------------------------------------
Title: Line shift, line asymmetry, and the ^6Li/^7Li isotopic ratio
    determination
Authors: Cayrel, R.; Steffen, M.; Chand, H.; Bonifacio, P.; Spite,
   M.; Spite, F.; Petitjean, P.; Ludwig, H. -G.; Caffau, E.
2007A&A...473L..37C    Altcode: 2007arXiv0708.3819C
  Context: Line asymmetries are generated by convective Doppler shifts in
  stellar atmospheres, especially in metal-poor stars, where convective
  motions penetrate to higher atmospheric levels. Such asymmetries are
  usually neglected in abundance analyses. The determination of the
  ^6Li/^7Li isotopic ratio is prone to suffering from such asymmetries,
  as the contribution of ^6Li is a slight blending reinforcement of the
  red wing of each component of the corresponding ^7Li line, with respect
  to its blue wing. <BR />Aims: The present paper studies the halo star
  HD 74000 and estimates the impact of convection-related asymmetries
  on the Li isotopic ratio determination. <BR />Methods: Two methods
  are used to meet this aim. The first, which is purely empirical,
  consists in deriving a template profile from another element that can
  be assumed to originate in the same stellar atmospheric layers as Li
  I, producing absorption lines of approximately the same equivalent
  width as individual components of the ^7Li I resonance line. The
  second method consists in conducting the abundance analysis based on
  NLTE line formation in a 3D hydrodynamical model atmosphere, taking
  into account the effects of photospheric convection. <BR />Results:
  The results of the first method show that the convective asymmetry
  generates an excess absorption in the red wing of the ^7Li absorption
  feature that mimics the presence of ^6Li at a level comparable to
  the hitherto published values. This opens the possibility that only
  an upper limit on ^6Li/^7Li has thus far been derived. The second
  method confirms these findings. <BR />Conclusions: From this work,
  it appears that a systematic reappraisal of former determinations of
  ^6Li abundances in halo stars is warranted. <P />Based on observations
  carried out at the European Southern Observatory (ESO), under prog. ID
  75.D-0600. Tables 1-3, and additional references are only available
  in electronic form at http://www.aanda.org

---------------------------------------------------------
Title: The evolution of planetary nebulae. IV. On the physics of
    the luminosity function
Authors: Schönberner, D.; Jacob, R.; Steffen, M.; Sandin, C.
2007A&A...473..467S    Altcode: 2007arXiv0708.4292S
  Context: The luminosity function of planetary nebulae, in use for
  about two decades in extragalactic distance determinations, is still
  subject to controversial interpretations. <BR />Aims: The physical
  basis of the luminosity function is investigated by means of several
  evolutionary sequences of model planetary nebulae computed with a 1D
  radiation-hydrodynamics code. <BR />Methods: The nebular evolution is
  followed from the vicinity of the asymptotic-giant branch across the
  Hertzsprung-Russell diagram until the white-dwarf domain is reached,
  using various central-star models coupled to different initial envelope
  configurations. Along each sequence the relevant line emissions of
  the nebulae are computed and analysed. <BR />Results: Maximum line
  luminosities in Hβ and [O iii] 5007 Å are achieved at stellar
  effective temperatures of about 65 000 K and 95 000...100 000 K,
  respectively, provided the nebula remains optically thick for ionising
  photons. In the optically thin case, the maximum line emission occurs
  at or shortly after the thick/thin transition. Our models suggest that
  most planetary nebulae with hotter (⪆ 45 000 K) central stars are
  optically thin in the Lyman continuum, and that their [O iii] 5007 Å
  emission fails to explain the bright end of the observed planetary
  nebulae luminosity function. However, sequences with central stars
  of ⪆0.6 M<SUB>⊙</SUB> and rather dense initial envelopes remain
  virtually optically thick and are able to populate the bright end
  of the luminosity function. Individual luminosity functions depend
  strongly on the central-star mass and on the variation of the nebular
  optical depth with time. <BR />Conclusions: Hydrodynamical simulations
  of planetary nebulae are essential for any understanding of the basic
  physics behind their observed luminosity function. In particular,
  our models do not support the claim of Marigo et al. (2004, A&amp;A,
  423, 995) according to which the maximum 5007 Å luminosity occurs
  during the recombination phase well beyond 100 000 K when the stellar
  luminosity declines and the nebular models become, at least partially,
  optically thick. Consequently, there is no need to invoke relatively
  massive central stars of, say &gt; 0.7 M<SUB>⊙</SUB>, to account
  for the bright end of the luminosity function. <P />Based in parts
  on observations <P />made with the NASA/ESA Hubble Space Telescope,
  obtained at the <P />Space Science Institute, which is operated by the
  Association of the <P />Universities for Research in Astronomy, Inc.,
  under NASA contract <P />NAS 5-26555. The data are retrieved from the
  ESO/ST-ECF Science Archive <P />Facility.

---------------------------------------------------------
Title: The PEPSI "deep spectrum" project
Authors: Steffen, Matthias; Strassmeier, Klaus G.
2007AN....328..632S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Inter-network regions of the Sun at millimetre wavelengths
Authors: Wedemeyer-Böhm, S.; Ludwig, H. G.; Steffen, M.; Leenaarts,
   J.; Freytag, B.
2007A&A...471..977W    Altcode: 2007arXiv0705.2304W
  Aims:The continuum intensity at wavelengths around 1 mm provides an
  excellent way to probe the solar chromosphere and thus valuable input
  for the ongoing controversy on the thermal structure and the dynamics of
  this layer. The synthetic continuum intensity maps for near-millimetre
  wavelengths presented here demonstrate the potential of future
  observations of the small-scale structure and dynamics of internetwork
  regions on the Sun. <BR />Methods: The synthetic intensity/brightness
  temperature maps are calculated on basis of three-dimensional
  radiation (magneto-)hydrodynamic (MHD) simulations. The assumption
  of local thermodynamic equilibrium (LTE) is valid for the source
  function. The electron densities are also treated in LTE for most maps
  but also in non-LTE for a representative model snapshot. Quantities
  like intensity contrast, intensity contribution functions, spatial
  and temporal scales are analysed in dependence on wavelength and
  heliocentric angle. <BR />Results: While the millimetre continuum
  at 0.3 mm originates mainly from the upper photosphere, the longer
  wavelengths considered here map the low and middle chromosphere. The
  effective formation height increases generally with wavelength and
  also from disk-centre towards the solar limb. The average intensity
  contribution functions are usually rather broad and in some cases they
  are even double-peaked as there are contributions from hot shock waves
  and cool post-shock regions in the model chromosphere. The resulting
  shock-induced thermal structure translates to filamentary brightenings
  and fainter regions in between. Taking into account the deviations from
  ionisation equilibrium for hydrogen gives a less strong variation of
  the electron density and with it of the optical depth. The result is
  a narrower formation height range although the intensity maps still
  are characterised by a highly complex pattern. The average brightness
  temperature increases with wavelength and towards the limb although
  the wavelength-dependence is reversed for the MHD model and the NLTE
  brightness temperature maps. The relative contrast depends on wavelength
  in the same way as the average intensity but decreases towards the
  limb. The dependence of the brightness temperature distribution on
  wavelength and disk-position can be explained with the differences in
  formation height and the variation of temperature fluctuations with
  height in the model atmospheres. The related spatial and temporal
  scales of the chromospheric pattern should be accessible by future
  instruments. <BR />Conclusions: Future high-resolution millimetre
  arrays, such as the Atacama Large Millimeter Array (ALMA), will
  be capable of directly mapping the thermal structure of the solar
  chromosphere. Simultaneous observations at different wavelengths
  could be exploited for a tomography of the chromosphere, mapping its
  three-dimensional structure, and also for tracking shock waves. The
  new generation of millimetre arrays will be thus of great value for
  understanding the dynamics and structure of the solar atmosphere.

---------------------------------------------------------
Title: Sulphur abundances from the S i near-infrared triplet at
    1045 nm
Authors: Caffau, E.; Faraggiana, R.; Bonifacio, P.; Ludwig, H. -G.;
   Steffen, M.
2007A&A...470..699C    Altcode: 2007arXiv0704.2335C
  Context: Unlike silicon and calcium, sulphur is an α-element
  that does not form dust. Some of the available observations of
  the evolution of sulphur with metallicity indicate an increased
  scatter of sulphur-to-iron ratios at low metallicities or even
  a bimodal distribution, with some stars showing constant S/Fe at
  all metallicities and others showing an increasing S/Fe ratio with
  decreasing metallicity. In metal-poor stars S i lines of Multiplet
  1 at 920 nm are not yet too weak to permit the measurement of the
  sulphur abundance A(S); however, in ground-based observations they
  are severely affected by telluric lines. <BR />Aims: We investigate
  the possibility of measuring sulphur abundances from S iMult. 3 at
  1045 nm lines. These lie in the near infrared and are slightly weaker
  than those of Mult. 1, but lie in a range not affected by telluric
  lines. <BR />Methods: We investigated the lines of Mult. 3 in the Sun
  (G2V), Procyon (F5V), HD 33256 (F5V), HD 25069 (G9V), and ɛ Eri (HD
  22049, K2V). For the Sun and Procyon the analysis was performed with
  CO^5BOLD 3D hydrodynamical model atmospheres, while the three other
  stars, for which hydrodynamical simulations are not available, were
  analysed using 1D model atmospheres. <BR />Results: For our sample of
  stars we find a global agreement between A(S) from lines of different
  multiplets. <BR />Conclusions: Our results suggest that the infrared
  lines of Mult. 3 are a viable indicator of the sulphur abundance
  that, because of the intrinsic strength of this multiplet, should be
  suitable for studying the trend of [S/Fe] at low metallicities. <P
  />Based on data from the UVES Paranal Observatory Project (ESO DDT
  Program ID 266.D-5655). Appendix is only available in electronic form
  at http://www.aanda.org

---------------------------------------------------------
Title: Spatially resolved spectroscopic studies of planetary nebulae
    and their halos
Authors: Sandin, C.; Schönberner, D.; Roth, M. M.; Steffen, M.;
   Böhm, P.; Monreal-Iber, A.
2007apn4.confE...6S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Internal Gravity Waves and their Role in the Energetics of
    the Solar Atmosphere
Authors: Fleck, Bernard; Straus, T.; Jefferies, S.; McIntosh, S. W.;
   Severino, G.; Steffen, M.
2007AAS...210.2410F    Altcode: 2007BAAS...39..130F
  Internal gravity waves are believed to be excited by convective
  overshoot in the solar atmosphere. We compare the results from numerical
  simulations of the overshoot region of compressible convection into a
  stable photosphere, with observations of the velocity field at several
  heights in the solar atmosphere. We find a consistent picture for the
  quiet middle/upper photosphere in which internal gravity waves are the
  dominant phenomenon at low frequencies (&lt; 2.5 mHz). We estimate the
  contribution of these waves to the energy balance in the photosphere
  and low chromosphere.

---------------------------------------------------------
Title: 3-D hydrodynamic simulations of convection in A stars
Authors: Kochukhov, O.; Freytag, B.; Piskunov, N.; Steffen, M.
2007IAUS..239...68K    Altcode: 2006astro.ph.10111K
  Broadening and asymmetry of spectral lines in slowly rotating late
  A-type stars provide evidence for high-amplitude convective motions. The
  properties of turbulence observed in the A-star atmospheres are not
  understood theoretically and contradict results of previous numerical
  simulations of convection. Here we describe an ongoing effort to
  understand the puzzling convection signatures of A stars with the
  help of 3-D hydrodynamic simulations. Our approach combines realistic
  spectrum synthesis and non-grey hydrodynamic models computed with the
  CO5BOLD code. We discuss these theoretical predictions and confront
  them with high-resolution spectra of A stars. Our models have, for
  the first time, succeeded in reproducing the observed profiles of weak
  spectral lines without introducing fudge broadening parameters.

---------------------------------------------------------
Title: Radiative hydrodynamics models of stellar convection
Authors: Steffen, Matthias
2007IAUS..239...36S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Carbon monoxide in the solar atmosphere. II. Radiative cooling
    by CO lines
Authors: Wedemeyer-Böhm, S.; Steffen, M.
2007A&A...462L..31W    Altcode: 2006astro.ph.12197W
  Aims: The role of carbon monoxide as a cooling agent for the thermal
  structure of the mid-photospheric to low-chromospheric layers of the
  solar atmosphere in internetwork regions is investigated. <BR />Methods:
  The treatment of radiative cooling via spectral lines of carbon
  monoxide (CO) has been added to the radiation chemo-hydrodynamics code
  CO5BOLD. The radiation transport has now been solved in a continuum band
  with Rosseland mean opacity and an additional band with CO opacity. The
  latter is calculated as a Planck mean over the CO band between 4.4
  and 6.2 μm. The time-dependent CO number density is derived from
  the solution of a chemical reaction network. <BR />Results: The CO
  opacity indeed causes additional cooling at the fronts of propagating
  shock waves in the chromosphere. There, the time-dependent approach
  results in a higher CO number density compared to the equilibrium
  case and hence in a larger net radiative cooling rate. The average
  gas temperature stratification of the model atmosphere, however, is
  only reduced by roughly 100 K. Also the temperature fluctuations and
  the CO number density are only affected to small extent. A numerical
  experiment without dynamics shows that the CO cooling process works in
  principle and drives the atmosphere to a cool radiative equilibrium
  state. At chromospheric heights, the radiative relaxation of the
  atmosphere to a cool state takes several 1000 s. The CO cooling process
  thus would seem to be too slow compared to atmospheric dynamics to be
  responsible for the very cool temperature regions observed in the solar
  atmosphere. <BR />Conclusions: . The hydrodynamical timescales in our
  solar atmosphere model are much too short to allow for the radiative
  relaxation to a cool state, thus suppressing the potential thermal
  instability due to carbon monoxide as a cooling agent. Apparently,
  the thermal structure and dynamics of the outer model atmosphere are
  instead determined primarily by shock waves.

---------------------------------------------------------
Title: 3D-Spectroscopy of Extragalactic Planetary Nebulae as
    Diagnostic Probes for Galaxy Evolution
Authors: Kelz, A.; Monreal-Ibero, A.; Roth, M. M.; Sandin, C.;
   Schönberner, D.; Steffen, M.
2007spts.conf..339K    Altcode: 2006astro.ph..7498K
  In addition to study extragalactic stellar populations in their
  integrated light, the detailed analysis of individual resolved
  objects has become feasible, mainly for luminous giant stars and for
  extragalactic planetary nebulae (XPNe) in nearby galaxies. A recently
  started project at the Astrophysical Institute Potsdam (AIP), called
  “XPN--Physics”, aims to verify if XPNe are useful probes to measure
  the chemical abundances of their parent stellar population. The project
  involves theoretical and observational work packages.

---------------------------------------------------------
Title: A First Three-Dimensional Model for the Carbon Monoxide
    Concentration in the Solar Atmosphere
Authors: Wedemeyer-Böhm, S.; Kamp, I.; Freytag, B.; Bruls, J.;
   Steffen, M.
2006ASPC..354..301W    Altcode:
  The time-dependent and self-consistent treatment of carbon monoxide
  (CO) has been added to the radiation chemo-hydrodynamics code
  CO5BOLD. It includes the solution of a chemical reaction network and
  the advection of the resulting particle densities with the hydrodynamic
  flow field. Here we present a first 3D simulation of the non-magnetic
  solar photosphere and low chromosphere, calculated with the upgraded
  code. In the resulting model, the highest amount of CO is located in
  the cool regions of the reversed granulation pattern in the middle
  photosphere. A large fraction of carbon is bound by CO throughout
  the chromosphere with exception of hot shock waves where the CO
  concentration is strongly reduced. The distribution of carbon monoxide
  is very inhomogeneous due to co-existing regions of hot and cool gas
  caused by the hydrodynamic flow. High-resolution observations of CO
  could thus provide important constraints for the thermal structure of
  the solar photosphere and chromosphere.

---------------------------------------------------------
Title: Detection of a Far-Infrared Bow Shock Nebula around R Hya:
    The First MIRIAD Results
Authors: Ueta, T.; Speck, A. K.; Stencel, R. E.; Herwig, F.; Gehrz,
   R. D.; Szczerba, R.; Izumiura, H.; Zijlstra, A. A.; Latter, W. B.;
   Matsuura, M.; Meixner, M.; Steffen, M.; Elitzur, M.
2006ApJ...648L..39U    Altcode: 2006astro.ph..7303U
  We present the first results of the MIRIAD (MIPS InfraRed Imaging
  of AGB Dust shells) project using the Spitzer Space Telescope. The
  primary aim of the project is to probe the material distribution in the
  extended circumstellar envelopes (CSEs) of evolved stars and recover
  the fossil record of their mass-loss history. Hence, we must map the
  whole of the CSEs plus the surrounding sky for background subtraction
  while avoiding the central star that is brighter than the detector
  saturation limit. With our unique mapping strategy, we have achieved
  better than 1 MJy sr<SUP>-1</SUP> sensitivity in 3 hr of integration
  and successfully detected a faint (&lt;5 MJy sr<SUP>-1</SUP>), extended
  (~400") far-infrared nebula around the asymptotic giant branch (AGB)
  star R Hya. Based on the parabolic structure of the nebula, the
  direction of the space motion of the star with respect to the nebula
  shape, and the presence of extended Hα emission cospatial to the
  nebula, we suggest that the detected far-IR nebula is due to a bow
  shock at the interface of the interstellar medium and the AGB wind
  of this moving star. This is the first detection of the stellar-wind
  bow shock interaction for an AGB star and exemplifies the potential
  of Spitzer as a tool to examine the detailed structure of extended
  far-IR nebulae around bright central sources.

---------------------------------------------------------
Title: Resonant Oscillation Modes and Background in Realistic
    Hydrodynamical Simulations of Solar Surface Convection
Authors: Straus, T.; Severino, G.; Steffen, M.
2006ESASP.617E...4S    Altcode: 2006soho...17E...4S
  No abstract at ADS

---------------------------------------------------------
Title: Working with VIMOS-IFU data: Searching and characterizing
    the faint haloes of planetary nebulae
Authors: Monreal-Ibero, A.; Roth, M. M.; Schönberner, D.; Steffen,
   M.; Böhm, P.
2006NewAR..50..426M    Altcode:
  In this contribution, we present the VIMOS-IFU data analysis of two
  planetary nebulae: NGC 3242 and NGC 4361. Due to the technical nature
  of the workshop, we emphasize some specific problems of data reduction
  and analysis: accuracy in flux calibration, importance of scattered
  light and improvement of the S/N ratio. We estimate that accuracy of
  our flux calibration is ∼15% in the spectral range 4200-6100 Å. At
  ∼10″ from the center of a point source, the intensity is ≲0.02%
  of the peak value, indicating that scattered light is negligible. Some
  examples of science that we are doing are shown. In particular, we
  have established an apparent temperature gradient across the halo of
  NGC NGC3242.

---------------------------------------------------------
Title: Nod &amp; Shuffle 3D Spectroscopy
Authors: Roth, Martin M.; Cardiel, Nicolas; Cenarro, Javier;
   Schönberner, Detlef; Steffen, Matthias
2006ASSL..336...99R    Altcode: 2006sda..conf...99R
  No abstract at ADS

---------------------------------------------------------
Title: The modelling of the X-ray emission of planetary nebulae
Authors: Schönberner, D.; Steffen, M.; Warmuth, A.
2006IAUS..234..161S    Altcode:
  We report on our recent efforts to compute the X-ray emission
  from the hot, shocked stellar wind gas filling the inner cavity
  of planetary nebulae. To this end, we updated our 1D hydrodynamics
  code NEBEL by including a module that computes the heat transfer by
  thermal conduction across the contact discontinuity separating the
  hot shocked wind gas from the much cooler nebular material. Given the
  temperature and density structure of the hot bubble the X-ray emission
  is computed by means of the CHIANTI code. We find a reasonably close
  agreement of the computed X-ray luminosities with recent observations
  of Newton-XMM and Chandra. Our simulations also predict how the X-ray
  emission depends on the wind luminosity and the stellar parameters.

---------------------------------------------------------
Title: 3D Spectroscopy — a powerful new tool for PN research
Authors: Roth, Martin M.; Schönberner, D.; Steffen, M.; Monreal,
   A.; Sandin, C.
2006IAUS..234...17R    Altcode:
  Historically, technological progress with detectors and instrumentation
  has been essential for advances in any field of observational
  astronomy, e.g. the advent of CCDs being crucial for high dynamic range
  imaging and quantitative spectroscopy of galactic PNe, faint object
  spectrophotometry for the discovery of extragalactic PNe to distances
  as far as 100 Mpc, etc. The emerging technique of integral field ("3D")
  spectroscopy, which is being applied quite successfully to extragalactic
  astronomy, has unfortunately hardly been used so far for the study of
  PNe. However, 3D spectroscopy has an enormous potential for various
  observational problems, ranging from high spatial resolution emission
  line mapping in different wavelengths simultaneously, over extremely
  high sensitivity spectroscopy of low surface brightness objects like
  e.g. PN haloes, to accurate 3D spectrophotometry of extragalactic PNe,
  and many others. As an attempt to encourage PN researchers to make
  better use of these new opportunities, the presently existing suite
  of 3D instruments on 4-8m class telescopes is reviewed, highlighting
  some examples of successful 3D observations for the study of PNe.

---------------------------------------------------------
Title: Hydrodynamical interpretation of basic nebular structures
Authors: Steffen, M.; Schönberner, D.
2006IAUS..234..285S    Altcode:
  Based on existing hydrodynamical simulations, we review our present
  understanding of the formation and evolution of planetary nebulae (PNe)
  and discuss the relevant processes responsible for the development of
  the basic (1D) nebular structures.

---------------------------------------------------------
Title: New observations of the halo radial temperature structure in
    NGC 7662
Authors: Sandin, C.; Schönberner, D.; Roth, M. M.; Steffen, M.;
   Monreal-Ibero, A.; Böhm, P.; Tripphahn, U.
2006IAUS..234..501S    Altcode: 2006astro.ph..9279S
  We report on our studies of the physical structure of the planetary
  nebula (PN) NGC 7662. Using (3D) Integral Field Spectroscopy we have
  been able to measure the electron temperature more accurately and at a
  larger number of radial locations than before. Here we briefly present
  our method by which we find a strong positive temperature gradient
  with increasing radius. According to hydrodynamic models a hot halo,
  when compared to the central star, can be the product of the passage
  of an ionization front (e.g. Marten 1993). Such a gradient is not
  found in equilibrium models, and this finding - when confirmed for
  other objects - strongly advocates the use of hydrodynamic models when
  modeling PN halos.

---------------------------------------------------------
Title: Crowded Field 3D Spectrophotometry of Extragalactic Planetary
    Nebulae
Authors: Roth, Martin M.; Becker, Thomas; Böhm, Petra; Schönberner,
   Detlef; Steffen, Matthias; Exter, Katrina
2006pnbm.conf..239R    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: On the luminosity function of planetary nebulae
Authors: Schönberner, D.; Jacob, R.; Steffen, M.
2006IAUS..234..505S    Altcode:
  A new assessment of the physics of the luminosity function of planetary
  nebulae is presented, based on our grid of nebular evolutionary
  sequences computed with a 1D radiation-hydrodynamics code. The nebular
  evolution is followed from the formation stage in the vicinity of the
  asymptotic-giant branch across the Hertzsprung-Russell diagram until the
  white-dwarf domain is reached, for various central-star models coupled
  to different initial envelope configurations. Along each sequence the
  relevant line luminosities of the nebulae are computed and analyzed. Our
  models predict that reasonably dense initial circumstellar envelopes
  with central stars of slightly above 0.6 M<SUB>⊙</SUB> will remain
  nearly optically thick and are able to provide the observed 5007 Å
  cutoff luminosity. We cannot support the claim of Marigo et al. (2004)
  according to which only planetary nebulae with central stars of &gt;
  0.7 M<SUB>⊙</SUB> are able to provide sufficient 5007 Å line emission
  to account for the bright end of the luminosity function.

---------------------------------------------------------
Title: Simulations of Magnetohydrodynamics and CO Formation from
    the Convection Zone to the Chromosphere
Authors: Wedemeyer-Böhm, S.; Schaffenberger, W.; Steiner, O.; Steffen,
   M.; Freytag, B.; Kamp, I.
2005ESASP.596E..16W    Altcode: 2005ccmf.confE..16W
  No abstract at ADS

---------------------------------------------------------
Title: On the Reliability of Planetary Nebulae as Extragalactic Probes
Authors: Schönberner, D.; Jacob, R.; Steffen, M.; Roth, M. M.
2005AIPC..804..269S    Altcode:
  We report on the first 1D radiation-hydrodynamics simulations aimed
  at exploring the metallicity dependance of the evolution of planetary
  nebulae. Using scaled mean abundances, based on Galactic disk objects,
  we found that for lower metallicities the nebulae become more dilute
  and prone to departures from thermal equilibrium because of the reduced
  wind power of the central star and the reduced cooling efficiency of
  the nebular gas. At selected evolutionary phases we `switched off'
  the hydrodynamic terms and computed equilibrium models for the fixed
  density structure and radiation field. This enabled us to study how
  the electron temperature and the emission of important diagnostic
  lines is influenced by hydrodynamics.

---------------------------------------------------------
Title: 3D Spectroscopy of Planetary Nebulae - Diagnostic Tools from
    the Milky Way to Nearby Galaxies and Beyond
Authors: Roth, Martin M.; Schönberner, Detlef; Steffen, Matthias;
   Monreal, Ana
2005AIPC..804...20R    Altcode:
  Integral field (“3D”) spectroscopy is an emerging observing
  technique in the process of becoming a common user tool, with a
  variety of powerful instruments becoming available at most major
  observatories. The application of this new method has a number of
  advantages over conventional techniques for both extended and point
  sources. We describe our experience with 3D spectroscopy applied to
  extremely low surface brightness regions in haloes of galactic planetary
  nebulae, and to extragalactic planetary nebulae in local group galaxies.

---------------------------------------------------------
Title: Searching and Characterizing the Faint Haloes of Planetary
Nebulae: A Study Case for Integral Field Spectroscopy
Authors: Monreal-Ibero, A.; Roth, M. M.; Schönberner, D.; Steffen,
   M.; Böhm, P.
2005AIPC..804..155M    Altcode:
  We present here the first results of a research project devoted to the
  characterization of the physical properties of the planetary nebulae
  haloes. We succeeded in determining some properties in the halo of
  NGC 3242, but we did not detect any halo feature down to the detection
  limit in NGC 4361.

---------------------------------------------------------
Title: Modeling X-ray Emission from Planetary Nebulae
Authors: Steffen, M.; Schönberner, D.; Warmuth, A.; Schwope, A.;
   Landi, E.; Perinotto, M.; Bucciantini, N.
2005AIPC..804..161S    Altcode:
  Recent observations using the Chandra X-ray Observatory and XXM Newton
  revealed without doubt diffuse X-ray emission from the shock-heated
  wind gas in planetary nebula (PN) interiors. Typical properties
  of the emitting gas are temperatures of a few 10<SUP>6</SUP> K and
  electron densities of the order of 100 cm<SUP>-3</SUP>. According
  to current hydrodynamical models, the shocked gas becomes too
  hot (T ~ 10<SUP>7</SUP>-10<SUP>8</SUP> K) and too tenuous (ne ~
  1 cm<SUP>-3</SUP>) to produce the observed X-ray emission. However,
  the hot gas is confined by the rather cool (T ~ 10 000K) nebular gas,
  and thermal heat conduction across the interface between the hot
  and cool gas becomes important. It changes the contact discontinuity
  into a more extended transition layer covering the temperature range
  where the observed X-ray emission is thought to arise. To date, only
  similarity solutions for the hydrodynamical problem of PN evolution
  with heat conduction have been derived (Zhekov &amp; Perinotto
  1996). We present first results from new numerical simulations of the
  PN evolution including thermal conduction by electrons. We confront
  the X-ray luminosities predicted by these models with those derived
  from XMM/Chandra observations.

---------------------------------------------------------
Title: The evolution of planetary nebulae. III. Internal kinematics
    and expansion parallaxes
Authors: Schönberner, D.; Jacob, R.; Steffen, M.
2005A&A...441..573S    Altcode:
  A detailed theoretical study of the basic internal kinematics of
  planetary nebulae is presented, based on 1D radiation-hydrodynamics
  simulations of circumstellar envelopes around central stars of 0.595
  and 0.696 M<SUB>⊙</SUB>. By means of observable quantities like
  radial surface-brightness distributions and emission-line profiles
  computed from the models, a comparison with real objects was performed
  and revealed a reasonable agreement. This allowed to draw important
  conclusions by investigating the kinematics of these models in
  detail. Firstly, it is shown that the determination of kinematical
  ages, normally considered to be simple if size and expansion rate of
  an object are given, can seriously be flawed. Secondly, the expansion
  law of a planetary nebula is different from what is assumed for
  deriving spatio-kinematical models. Thirdly and most importantly, our
  hydrodynamical models help to correctly use existing angular expansion
  measurements for distance determinations. The mere combination of the
  angular expansion rates with the spectroscopic expansion velocities
  leads always to a serious underestimate of the distance, the degree
  of which depends on the evolutionary state of the object. The
  necessary correction factor varies between 3 and 1.3. Individual
  correction factors can be estimated with an accuracy of about 10%
  by matching our hydrodynamical models to real objects. As a result,
  revised distances for a few objects with reliable angular expansion
  rates are presented. But even these corrected distances are not always
  satisfying: they still appear to be inconsistent with other distance
  determinations and, even more disturbing, with the accepted theory of
  post-asymptotic giant branch evolution. As a byproduct of the angular
  expansion measurements, the transition times from the vicinity of
  the asymptotic giant branch to the planetary-nebula regime could
  be estimated. They appear to be shorter than assumed in the present
  evolutionary calculations.

---------------------------------------------------------
Title: Integral Field Spectroscopy of Faint Halos of Planetary Nebulae
Authors: Monreal-Ibero, A.; Roth, M. M.; Schönberner, D.; Steffen,
   M.; Böhm, P.
2005ApJ...628L.139M    Altcode: 2005astro.ph..6300M
  We present the first integral field spectroscopy observations of the
  two planetary nebulae NGC 3242 and NGC 4361 with the VIMOS instrument
  attached to VLT-UT3. By co-adding a large number of spaxels, we
  reach an emission-line detection limit of 5×10<SUP>-18</SUP> ergs
  cm<SUP>-2</SUP> s<SUP>-1</SUP> arcsec<SUP>-2</SUP>. In the case of NGC
  3242, we succeed in determining some properties of the halo. The radial
  surface brightness profile in [O III] implies increasing mass loss
  before the formation of the planetary nebula. Traces of the mysterious
  “rings” are clearly visible. We find for the first time an apparent
  temperature gradient across a halo: from about 16,000 K close to the
  shell/halo transition to 20,000 K at the halo's outer edge. No line
  emission is seen in the suspected halo region of NGC 4361 down to the
  sensitivity limit.

---------------------------------------------------------
Title: MIPS Infrared Imaging of AGB Dustshells (MIRIAD): tracing
    mass-loss histories in the extremely large shells around evolved stars
Authors: Speck, Angela; Elitzur, Moshe; Gehrz, Robert; Herwig, Falk;
   Izumiura, Hideyuki; Latter, William; Matsuura, Mikako; Meixner,
   Margaret; Steffen, Matthias; Stencel, Robert; Szczerba, Ryszard;
   Ueta, Toshiya; Zijlstra, Albert
2005sptz.prop20258S    Altcode:
  Evolved intermediate mass stars are major contributors to the
  interstellar medium. However, the mechanisms by which they do this
  are not well understood. The circumstellar shells of evolved stars
  (AGB and post-AGB stars) contain the fossil record of their mass
  loss, and therefore have the potential to verify many aspects of
  stellar evolution. IRAS and ISO data indicate that huge dust shells
  exist around many such objects, extending several parsecs from the
  central star. Furthermore, these large dust shells show evidence
  for mass-loss variations that correlate with evolutionary changes
  in the star itself. Previous observations lacked the sensitivity
  and spatial resolution to investigate the full extent and detailed
  structure of these large dust shells. Using Spitzer/MIPS's unique
  sensitivity and mapping capabilities, we propose to produce far-IR
  images of the parsec-sized dust shells around four carefully selected
  evolved stars in order to determine the distribution of material in
  these circumstellar envelopes. These maps will be the deepest yet
  (sensitivity 1MJy/sr) and have the most complete spatial coverage to
  date. Crucially, mapping in this level of detail will allow us to:
  (a) constrain the masses of the progenitor stars; (b) test theories of
  stellar evolution and mass-loss mechanisms; (c) determine the effect
  of dust chemistry on mass loss (and therefore on stellar evolution);
  (d) determine when the aspherical structures so prevalent in planetary
  nebulae actually develop and thus constrain the cause.

---------------------------------------------------------
Title: Science with the STELLA robotic observatory
Authors: Weber, M.; Strassmeier, K. G.; Bartus, J.; Korhonen, H.;
   Kővári, Zs.; Oláh, K.; Schwope, A.; Staude, A.; Steffen, M.
2005ESASP.560.1025W    Altcode: 2005csss...13.1025W
  No abstract at ADS

---------------------------------------------------------
Title: The shock-patterned solar chromosphere in the light of ALMA
Authors: Wedemeyer-Böhm, S.; Ludwig, H. -G.; Steffen, M.; Freytag,
   B.; Holweger, H.
2005ESASP.560.1035W    Altcode: 2005csss...13.1035W; 2005astro.ph..9747W
  Recent three-dimensional radiation hydrodynamic simulations by Wedemeyer
  et al. (2004) suggest that the solar chromosphere is highly structured
  in space and time on scales of only 1000 km and 20-25 sec, resp.. The
  resulting pattern consists of a network of hot gas and enclosed cool
  regions which are due to the propagation and interaction of shock
  fronts. In contrast to many other diagnostics, the radio continuum at
  millimeter wavelengths is formed in LTE, and provides a rather direct
  measure of the thermal structure. It thus facilitates the comparison
  between numerical model and observation. While the involved time
  and length scales are not accessible with todays equipment for that
  wavelength range, the next generation of instruments, such as the
  Atacama Large Millimeter Array (ALMA), will provide a big step towards
  the required resolution. Here we present results of radiative transfer
  calculations at mm and sub-mm wavelengths with emphasis on spatial
  and temporal resolution which are crucial for the ongoing discussion
  about the chromospheric temperature structure.

---------------------------------------------------------
Title: 3D simulation of convection and spectral line formation in
    A-type stars
Authors: Steffen, M.; Freytag, B.; Ludwig, H. -G.
2005ESASP.560..985S    Altcode: 2005astro.ph..9464S; 2005csss...13..985S
  We present first realistic numerical simulations of 3D radiative
  convection in the surface layers of main sequence A-type stars with Teff
  = 8000 K and 8500 K, log g = 4.4 and 4.0, recently performed with the
  CO5BOLD radiation hydrodynamics code. The resulting models are used to
  investigate the structure of the H+HeI and the HeII convection zones
  in comparison with the predictions of local and non-local convection
  theories, and to determine the amount of "overshoot" into the stable
  layers below the HeII convection zone. The simulations also predict
  how the topology of the photospheric granulation pattern changes from
  solar to A-type star convection. The influence of the photospheric
  temperature fluctuations and velocity fields on the shape of spectral
  lines is demonstrated by computing synthetic line profiles and line
  bisectors for some representative examples, allowing us to confront
  the 3D model results with observations.

---------------------------------------------------------
Title: The evolution of planetary nebulae.  II. Circumstellar
    environment and expansion properties
Authors: Schönberner, D.; Jacob, R.; Steffen, M.; Perinotto, M.;
   Corradi, R. L. M.; Acker, A.
2005A&A...431..963S    Altcode:
  We investigate and discuss the expansion properties of planetary nebulae
  by means of 1D radiation-hydrodynamics models computed for different
  initial envelope configurations and central star evolutionary tracks. In
  particular, we study how the expansion depends on the initial density
  gradient of the circumstellar envelope and show that it is possible
  to derive information on the very last mass-loss episodes during the
  star's final evolution along and off the asymptotic giant branch. To
  facilitate the comparison of the models with real objects, we have also
  computed observable quantities like surface brightness and emission-line
  profiles. With the help of newly acquired high-resolution emission-line
  profiles for a sample of planetary nebulae we show that models with
  initial envelopes based on the assumption of a stationary wind outflow
  fail to explain the observed expansion speeds of virtually all of the
  observed planetary nebulae. Instead it must be assumed that during the
  very last phase of evolution along the final asymptotic giant branch
  evolution the mass-loss rate increases in strength, resulting in a much
  steeper slope of the circumstellar radial density distribution. Under
  these conditions, the expansion properties of the nebular gas differ
  considerably from the self-similar solutions found for isothermal
  conditions. Furthermore, the mass loss must remain at a rather high
  level until the stellar remnant begins to evolve quickly towards the
  central star regime. Current theoretical computations of dust-driven
  mass-loss which are restricted to rather low temperatures cannot be
  applied during the star's departure from the asymptotic giant branch. <P
  />Based on observations obtained at the 3.5 μm NTT and the 1.2 μm CAT
  telescope of the European Southern Observatory, La Silla, and at the
  2.6 μm NOT telescope operated on the island of La Palma by NOTSA, in
  the Spanish Observatorio del Roque de Los Muchachos of the Institutode
  Astrofísica de Canarias. <P />Dedicated to Prof. V. Weidemann on the
  occasion of his 80th birthday, October 3, 2004.

---------------------------------------------------------
Title: Numerical simulations of convection in A-stars
Authors: Freytag, Bernd; Steffen, Matthias
2004IAUS..224..139F    Altcode:
  Radiation hydrodynamics simulations have been used to produce numerical
  models of the convective surface layers of a number of stars, including
  the Sun and other stars on or above the main-sequence, white dwarfs
  of type DA, and red supergiants.

---------------------------------------------------------
Title: Ionization and its Structural Impacts on the Evolution of
    Planetary Nebulae
Authors: Schönberner, D.; Steffen, M.; Jacob, R.
2004ASPC..313..283S    Altcode: 2004apnw.conf..283S
  We review our present knowledge about the formation and evolution
  of planetary nebulae and evaluate the relative importance of
  photoionization and wind interaction. It turns out that heating by
  photoionization drives the expansion of a planetary nebula during
  its entire life, while wind interaction accelerates and shapes the
  inner regions only during the later stages of evolution. We found
  observational evidence that the transition from spherical AGB-wind
  structures to more aspherical ones must occur when the star begins to
  evolve slowly off the AGB.

---------------------------------------------------------
Title: The evolution of planetary nebulae. I. A
    radiation-hydrodynamics parameter study
Authors: Perinotto, M.; Schönberner, D.; Steffen, M.; Calonaci, C.
2004A&A...414..993P    Altcode:
  We follow hydrodynamically the evolution of spherimodel planetary
  nebulae subject to different initial conditions and with various
  central stars, investigating how combinations of central-star
  mass and asymptotic giant branch mass-loss rate determine the
  shape and kinematics of a planetary nebula. With this approach we
  aim at constituting a framework useful for the interpretation of
  the evolutionary status and previous mass-loss history of observed
  individual nebulae, making use of their kinematiproperties and surface
  brightness characteristics. In particular, the models are compared with
  the observed morphologies and kinematics of double shell nebulae. The
  dynamical structure of all the models is characterized by a more or
  less complicated shock wave pattern set up by ionization and wind
  interaction whose combined action results in general in a typical
  double-shell structure. We have found that models with simple initial
  structures based on a constant AGB mass-loss rate fail to comply with
  observed shell morphologies and surface-brightness distributions. A
  reasonable agreement with the observations is only found for a model
  where the mass-loss rate is strongly increasing towards the end of the
  asymptotic giant-branch evolution. Depending on the central star's
  evolutionary speed and the density of the cool wind expelled along
  the asymptotic giant-branch, planetary nebulae may never get optically
  thin. This is primarily the case for the more massive central stars,
  and this fact offers a rather natural explanation for the long standing
  problem of the very existence of molecular hydrogen in the immediate
  vicinity of hot central stars. We also show that distances to planetary
  nebulae based on expansion parallaxes are systematically too small by
  a significant amount.

---------------------------------------------------------
Title: Numerical simulation of the three-dimensional structure and
    dynamics of the non-magnetic solar chromosphere
Authors: Wedemeyer, S.; Freytag, B.; Steffen, M.; Ludwig, H. -G.;
   Holweger, H.
2004A&A...414.1121W    Altcode: 2003astro.ph.11273W
  Three-dimensional numerical simulations with CO<SUP>5</SUP>, a
  new radiation hydrodynamics code, result in a dynamic, thermally
  bifurcated model of the non-magnetic chromosphere of the quiet Sun. The
  3D model includes the middle and low chromosphere, the photosphere,
  and the top of the convection zone, where acoustic waves are excited
  by convective motions. While the waves propagate upwards, they steepen
  into shocks, dissipate, and deposit their mechanienergy as heat in
  the chromosphere. Our numerical simulations show for the first time
  a complex 3D structure of the chromospheric layers, formed by the
  interaction of shock waves. Horizontal temperature cross-sections of
  the model chromosphere exhibit a network of hot filaments and enclosed
  cool regions. The horizontal pattern evolves on short time-scales of
  the order of typically 20-25 s, and has spatial scales comparable to
  those of the underlying granulation. The resulting thermal bifurcation,
  i.e., the co-existence of cold and hot regions, provides temperatures
  high enough to produce the observed chromospheric UV emission and -
  at the same time - temperatures cold enough to allow the formation
  of molecules (e.g., carbon monoxide). Our 3D model corroborates the
  finding by \citet{carlsson94} that the chromospheric temperature rise
  of semi-empirical models does not necessarily imply an increase in
  the average gas temperature but can be explained by the presence of
  substantial spatial and temporal temperature inhomogeneities.

---------------------------------------------------------
Title: On the expansion parallaxes of planetary nebulae.
Authors: Schoenberner, D.; Jacob, R.; Steffen, M.
2004ANS...325..105S    Altcode: 2004ANS...325a.105S; 2004ANS...325..P37S
  No abstract at ADS

---------------------------------------------------------
Title: Spectroscopy of extragalactic planetary nebulae as tracers
    of intermediate age and old stellar populations.
Authors: Roth, M. M.; Schoenberner, D.; Steffen, M.; Becker, T.
2004ANS...325...46R    Altcode: 2004ANS...325..F09R; 2004ANS...325a..46R
  No abstract at ADS

---------------------------------------------------------
Title: Probing the mass-loss history at the tip of the AGB by
    planetary nebulae.
Authors: Schoenberner, D.; Jacob, R.; Hildebrandt, G.; Steffen, M.;
   Lehmann, H.; Corradi, R.; Acker, A.
2004ANS...325..104S    Altcode: 2004ANS...325..P36S; 2004ANS...325a.104S
  No abstract at ADS

---------------------------------------------------------
Title: 3D Simulation of the Solar Granulation: A Comparison of two
    Different Hydrodynamics Codes
Authors: Steffen, Matthias; Ludwig, Hans-Günter; Freytag, Bernd
2003ANS...324..174S    Altcode: 2003ANS...324..P96S
  No abstract at ADS

---------------------------------------------------------
Title: Modelling the Chromospheric Background Pattern of the
    Non-magnetic Sun
Authors: Wedemeyer, Sven; Freytag, Bernd; Steffen, Matthias; Ludwig,
   Hans-Günter; Holweger, Hartmut
2003ANS...324R..66W    Altcode: 2003ANS...324..I07W
  No abstract at ADS

---------------------------------------------------------
Title: Long Term Modeling of Mass Loss on the Late AGB
Authors: Simis, Yvonne; Schonberner, Detlef; Steffen, Matthias
2003ANS...324...18S    Altcode: 2003ANS...324..D03S; 2003ANS...324b..18S
  No abstract at ADS

---------------------------------------------------------
Title: Ionized haloes in planetary nebulae: new discoveries,
    literature compilation and basic statistical properties
Authors: Corradi, R. L. M.; Schönberner, D.; Steffen, M.; Perinotto,
   M.
2003MNRAS.340..417C    Altcode:
  We present a comprehensive observational study of haloes around
  planetary nebulae (PNe). Deep Hα+[NII] and/or [OIII] narrow-band
  images have been obtained for 35 PNe, and faint extended haloes have
  been newly discovered in the following 10 objects: Cn 1-5, IC 2165,
  IC 2553, NGC 2792, NGC 2867, NGC 3918, NGC 5979, NGC 6578, PB 4, and
  possibly IC 1747. New deep images have also been obtained of other
  known or suspected haloes, including the huge extended emission around
  NGC 3242 and Sh 2-200. In addition, the literature was searched, and
  together with the new observations an improved data base containing
  some 50 PN haloes has been compiled. <P />The halo sample is illustrated
  in an image atlas contained in this paper, and the original images are
  made available for use by the scientific community at &lt;externallink
  type="url"&gt;http://www.ing. iac.es/~rcorradi/HALOES/&lt;/A&gt;. <P
  />The haloes have been classified following the predictions of modern
  radiation-hydrodynamical simulations that describe the formation and
  evolution of ionized multiple shells and haloes around PNe. According
  to the models, the observed haloes have been divided into the following
  groups: (i) circular or slightly elliptical asymptotic giant branch
  (AGB) haloes, which contain the signature of the last thermal pulse
  on the AGB; (ii) highly asymmetrical AGB haloes; (iii) candidate
  recombination haloes, i.e. limb-brightened extended shells that are
  expected to be produced by recombination during the late post-AGB
  evolution, when the luminosity of the central star drops rapidly by a
  significant factor; (iv) uncertain cases which deserve further study
  for a reliable classification; (v) non-detections, i.e. PNe in which
  no halo is found to a level of &lt;~10<SUP>-3</SUP> the peak surface
  brightness of the inner nebulae. <P />We discuss the properties of the
  haloes: detection rate, morphology, location of the central stars in
  the Hertzsprung-Russell diagram, sizes, surface brightness profiles,
  and kinematical ages. Among the most notable results, we find that, as
  predicted by models, ionized AGB haloes are a quite common phenomenon
  in PNe, having been found in 60 per cent of elliptical PNe for which
  adequately deep images exist. Another 10 per cent show possible
  recombination haloes. In addition, using the kinematical ages of
  the haloes and inner nebulae, we conclude that most of the PNe with
  observed AGB haloes have left the AGB far from a thermal pulse, at a
  phase when hydrogen burning is the dominant energy source. We find no
  significant differences between the AGB haloes of hydrogen-poor and
  hydrogen-rich central stars.

---------------------------------------------------------
Title: Formation and Evolution of Planetary Nebulae: A Radiation
    Hydrodynamics Study
Authors: Perinotto, M.; Calonaci, C.; Schönberner, D.; Steffen, M.;
   Blöcker, T.
2003IAUS..209..157P    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: AGB Mass-Loss History and Haloes Around Planetary Nebulae
Authors: Corradi, R. L. M.; Steffen, M.; Schönberner, D.; Perinotto,
   M.
2003IAUS..209..455C    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: From Red Giants to White Dwarfs -- A Radiation-Hydrodynamics
    Simulation of the Planetary Nebula Stage
Authors: Schönberner, D.; Steffen, M.
2003ASIB..105...19S    Altcode: 2003whdw.conf...19S; 2003whsw.conf...19S
  Based on 1D radiation-hydrodynamics simulations along the upper AGB we
  followed the evolution of AGB wind envelopes towards the white dwarf
  domain. Taking into account photoionization and wind interaction in
  a realistic manner, the hydrodynamics of the post-AGB phase leads,
  if coupled to an evolving 0.6 M<SUB>odot</SUB> central star model, to
  morphologies very similar to what is observed for spherical/elliptical
  planetary nebulae.

---------------------------------------------------------
Title: Structure and Evolution of Planetary Nebula Haloes
Authors: Steffen, M.; Schönberner, D.
2003IAUS..209..439S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Acoustic Waves in the Solar Chromosphere - Numerical
    Simulations with COBOLD
Authors: Wedemeyer, S.; Freytag, B.; Steffen, M.; Ludwig, H. -G.;
   Holweger, H.
2003IAUS..210P..C1W    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: 3-D hydrodynamic simulations of the solar chromosphere
Authors: Wedemeyer, S.; Freytag, B.; Steffen, M.; Ludwig, H. -G.;
   Holweger, H.
2003AN....324..410W    Altcode:
  We present first results of three-dimensional numerical simulations
  of the non-magnetic solar chromosphere, computed with the radiation
  hydrodynamics code CO<SUP>5</SUP>BOLD. Acoustic waves which are
  excited at the top of the convection zone propagate upwards into the
  chromosphere where the waves steepen into shocks. The interaction of
  the waves leads to the formation of complex structures which evolve
  on short time scales. Consequently, the model chromosphere is highly
  dynamical, inhomogeneous, and thermally bifurcated.

---------------------------------------------------------
Title: The Formation and Evolution of Planetary Nebulae (invited
    review)
Authors: Schönberner, D.; Steffen, M.
2003IAUS..209..147S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Granulation Abundance Corrections from Hydrodynamical
    Convection Simulations
Authors: Steffen, M.; Holweger, H.
2003IAUS..210P.D15S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Spots on the surface of Betelgeuse --  Results from new 3D
    stellar convection models
Authors: Freytag, B.; Steffen, M.; Dorch, B.
2002AN....323..213F    Altcode:
  The observed irregular brightness fluctuations of the well-known red
  supergiant Betelgeuse (alpha Ori, M2 Iab) have been attributed by
  M. Schwarzschild (1975) to the changing granulation pattern formed
  by only a few giant convection cells covering the surface of this
  giant star. The surface structure revealed by modern interferometric
  methods appears to be generally consistent with the explanation as
  large-scale granular intensity fluctuations. The interferometric
  data can be modeled equally well by assuming the presence of a few
  (up to 3) unresolved hot or cool spots on a limb-darkened disk. In an
  effort to improve our theoretical understanding of the Betelgeuse
  phenomena, we have applied a new radiation hydrodynamics code
  (CO<SUP>5</SUP>BOLD) to the problem of global convection in giant
  stars. For this purpose, the "local box" setup usually employed for the
  simulation of solar-type surface convection cannot be used. Rather, we
  have chosen a radically different approach: the whole star is enclosed
  in a cube ("star-in-a-box" setup). The properties of the stellar model
  are defined by the prescribed gravitational central potential and by
  a special inner boundary condition which replaces the unresolved core,
  including the source of nuclear energy production. We present current
  results obtained from this novel generation of 3D stellar convection
  simulations, proceeding from a toy model ("Mini-Sun") towards the
  numerically more demanding supergiant regime. We discuss the basic
  observational properties of Betelgeuse in the light of our best model
  obtained so far (T_eff = 3300 K, log g = -0.4). Finally, we describe a
  first attempt to investigate the interaction of the global convective
  flows with magnetic fields based on the kinematic approximation.

---------------------------------------------------------
Title: Line formation in convective stellar
    atmospheres. I. Granulation corrections for solar photospheric
    abundances
Authors: Steffen, M.; Holweger, H.
2002A&A...387..258S    Altcode: 2002astro.ph..3127S
  In an effort to estimate the largely unknown effects of photospheric
  temperature fluctuations on spectroscopic abundance determinations, we
  have studied the problem of LTE line formation in the inhomogeneous
  solar photosphere based on detailed 2-dimensional radiation
  hydrodynamics simulations of the convective surface layers of the
  Sun. By means of a strictly differential 1D/2D comparison of the
  emergent equivalent widths, we have derived “granulation abundance
  corrections” for individual lines, which have to be applied to
  standard abundance determinations based on homogeneous 1D model
  atmospheres in order to correct for the influence of the photospheric
  temperature fluctuations. In general, we find a line strengthening in
  the presence of temperature inhomogeneities as a consequence of the
  non-linear temperature dependence of the line opacity. The resulting
  corrections are negligible for lines with an excitation potential around
  E<SUB>i</SUB>=5 eV, regardless of element and ionization stage. Moderate
  granulation effects (Delta<SUB>gran</SUB> ~ -0.1 dex) are obtained
  for weak, high-excitation lines (E<SUB>i</SUB> &gt;~ 10 eV) of C I,
  N I, O I as well as Mg II and Si II. The largest corrections are found
  for ground state lines (E<SUB>i</SUB>=0 eV) of neutral atoms with an
  ionization potential between 6 and 8 eV like Mg I, Ca I, Ti I, Fe I,
  amounting to Delta_gran ~ -0.3 dex in the case of Ti I. For many lines
  of practical relevance, the magnitude of the abundance correction may
  be estimated from interpolation in the tables and graphs provided with
  this paper. The application of abundance corrections may often be an
  acceptable alternative to a detailed fitting of individual line profiles
  based on hydrodynamical simulations. The present study should be helpful
  in providing upper bounds for possible errors of spectroscopic abundance
  analyses, and for identifying spectral lines which are least sensitive
  to the influence of photospheric temperature inhomogeneities.

---------------------------------------------------------
Title: Planetary Nebulae with Double Shells and Haloes: Insights
    from Hydrodynamical Simulations
Authors: Schönberner, D.; Steffen, M.
2002RMxAC..12..144S    Altcode:
  We combined hydrodynamical simulations with stellar evolutionary
  calculations based on prescribed mass-loss rates in order to get a
  better understanding of how structure and kinematics of circumstellar
  matter develop with time during the late AGB and the following post-AGB
  and Planetary Nebula (PN) evolution.

---------------------------------------------------------
Title: Habitable zones in extrasolar planetary systems
Authors: Franck, Siegfried; von Bloh, Werner; Bounama, Christine;
   Steffen, Matthias; Schönberner, Detlef; Schellnhuber, Hans-Joachim
2002abqc.book...47F    Altcode:
  Summarizing we can state that the habitable zone (HZ) is the range
  of orbital distances from a star, in which a planet can maintain
  liquid water and biological productivity on its surface. The HZ can
  be calculated with the help of climatological approaches or within
  the framework of Earth system science. According to our model, the
  HZ for the present solar system extends between about 0.95 AU and
  about 1.2 AU and was broader in the past. For extrasolar systems we
  can postulate a distinct HZ for young central stars in the mass range
  between about 0.4 and 2 solar masses. The next two parts describe model
  calculations for the Sun and for other single main sequence stars,
  respectively. In the final we give our main conclusions and point out
  several areas for future work.

---------------------------------------------------------
Title: Habitable Zones and the Number of Gaia's Sisters
Authors: Franck, S.; von Bloh, W.; Bounama, C.; Steffen, M.;
   Schönberner, D.; Schellnhuber, H. -J.
2002ASPC..269..261F    Altcode: 2002esip.conf..261F
  No abstract at ADS

---------------------------------------------------------
Title: Spectroscopic influence of temperature inhomogeneities
Authors: Cayrel, Roger; Steffen, Matthias
2002HiA....12..423C    Altcode:
  The effect of temperature inhomogeneities on the formation of two
  oxygen lines and one Fe II line has been investigated based on 2-D
  radiation hydrodynamics simulations of convection in the atmospheres
  of metal-poor stars. It was expected that the IR O I triplet lines
  would be enhanced by the temperature inhomogeneities, more than the
  forbidden [O I] line or Fe II lines. The actual computations done on
  two snapshots under the assumption of LTE have not confirmed this
  expectation, instead suggesting that the main difference between
  "classical" and "dynamical" atmospheres of metal-poor dwarfs is the
  significantly cooler mean temperature of the dynamical upper photosphere
  (τ<SUB>Ross</SUB>&lt;~0.01).

---------------------------------------------------------
Title: The Evolution of AGB Stars Towards Planetary Nebulae
Authors: Schönberner, Detlef; Steffen, Matthias
2001ASSL..265...85S    Altcode: 2001pao..conf...85S
  We combined hydrodynamical simulations with stellar evolutionary
  calculations based on prescribed mass-loss rates in order to get a
  better understanding of how structure and kinematics of circumstellar
  matter develop with time during the late AGB and the following
  post-AGB evolution. We show (i) that the final density profile of
  the circumstellar shells produced by AGB mass loss falls off steeper
  than ρ ~r<SUP>-2</SUP>, (ii) that stages of high mass-loss rates are
  periodically interrupted by shorter phases of much lower outflow rates
  and speeds due to the luminosity dips associated with thermal pulses,
  and (iii) that during the post-AGB evolution ionization destroys the
  initial density and velocity distribution set up at the end of the AGB.

---------------------------------------------------------
Title: Evolution of Thin Gas Shells Along the AGB and Beyond
Authors: Steffen, Matthias; Schönberner, Detlef
2001ASSL..265..131S    Altcode: 2001pao..conf..131S
  Based on numerical simulations with two different computer codes,
  we have studied the time-dependent hydrodynamics of circumstellar
  gas/dust shells of AGB stars in their final stages of evolution. We
  discuss two different mechanisms capable of producing very thin shells
  of greatly enhanced gas density in the dusty outflows from these stars
  and illustrate their observable signatures. Our model calculations
  demonstrate that the thin shells produced on the AGB survive the
  transition to the post-AGB phase and can still be detected in the
  haloes of some Planetary Nebulae.

---------------------------------------------------------
Title: Acoustic Energy Generated by Convection: 3-D Numerical
    Simulations for the Sun
Authors: Wedemeyer, Sven; Freytag, Bernd; Holweger, Hartmut; Ludwig,
   Hans-Günter; Steffen, Matthias
2001AGM....18..P01W    Altcode:
  Dissipation of acoustic waves may be an efficient heating mechanism for
  the lower and middle chromosphere of the quiet Sun. The basic idea is
  that turbulent motions at the top of the solar convection zone generate
  acoustic waves which propagate upwards and dissipate in the lower and
  middle chromosphere, transporting energy into the higher layers. But
  still the question remains if this amount of energy is sufficient to
  explain the observed temperature increase without invoking magnetic
  fields. With a new version of the COBOLD radiation hydrodynamics code
  we are able to compute 3-D models extending all the way from the upper
  convection zone to the middle chromosphere. First 3-D simulations reveal
  a complex, inhomogenous and highly dynamical structure of the lower and
  middle chromosphere which evolves on rather short timescales. On small
  spatial dimensions very cool regions are present next to a "network"
  of hotter matter. The code is being developed further to provide a
  more detailed analysis and comparison with observations.

---------------------------------------------------------
Title: Limits of photosynthesis in extrasolar planetary systems for
    earth-like planets
Authors: Franck, S.; von Bloh, W.; Bounama, C.; Steffen, M.;
   Schönberner, D.; Schellnhuber, H. J.
2001AdSpR..28..695F    Altcode:
  We present a general modeling scheme for investigating the possibility
  of photosynthesis-based life on extrasolar planets. The scheme focuses
  on the identification of the habitable zone in main-sequence-star
  planetary systems with planets of Earth mass and size. Our definition
  of habitability is based on the long-term possibility of photosynthetic
  biomass production as a function of mean planetary surface temperature
  and atmospheric CO <SUB>2</SUB>-content. All the astrophysical,
  climatological, biogeochemical, and geodynamic key processes involved
  in the generation of photosynthesis-driven life conditions are taken
  into account. Implicitly, a co-genetic origin of the central star and
  the orbiting planet is assumed. The numerical solution of an advanced
  geodynamic model yields realistic look-up diagrams for determining the
  limits of photosynthesis in extrasolar planetary systems, assuming
  minimum CO <SUB>2</SUB> levels set by the demand of C <SUB>4</SUB>
  photosynthesis.

---------------------------------------------------------
Title: Extrasolar Planetary Habitable Zones and the Number of Gaias
Authors: von Bloh, W.; Franck, S.; Bounama, C.; Steffen, M.;
   Schönberner, D.; Schellnhuber, H. -J.
2001AGM....18..P35V    Altcode:
  We present a general modelling scheme for assessing the suitability for
  life on any Earth-like extrasolar planet by calculating the habitable
  zone (HZ) in main-sequence-star planetary systems. Our approach is based
  on an integrated Earth system analysis that relates the boundaries
  of the HZ to the limits of C4-photosynthesis processes. Within this
  model, the evolution of the HZ for any main-sequence-star planetary
  system can be calculated straightforwardly, and a convenient filter
  can be constructed that picks the candidates for photosynthesis-based
  life from all the extrasolar planets discovered by novel observational
  methods. These results can be used to determine the average number of
  planets per planetary system that are within the HZ. With the help
  of a segment of the Drake equation, the number of “Gaias” (i.e.,
  extrasolar terrestrial planets with a globally acting biosphere) can
  be estimated. Our calculation gives about half a million Gaias in the
  Milky Way.

---------------------------------------------------------
Title: Numerical Simulation of Stellar Convection: Comparison with
    Mixing-length Theory
Authors: Steffen, M.; Jordan, S.
2000eaa..bookE5198S    Altcode:
  The energy released by nuclear fusion in the STELLAR INTERIOR
  is carried to the surface by two different transport mechanisms,
  radiation and convection. In the presence of a temperature gradient,
  there is always a net radiative energy flux since more photons travel
  from hot to cool regions than in the other direction. If the temperature
  gradient exceeds a certain t...

---------------------------------------------------------
Title: On the origin of thin detached gas shells around AGB
    stars. Insights from time-dependent hydrodynamical simulations
Authors: Steffen, M.; Schönberner, D.
2000A&A...357..180S    Altcode:
  We have applied two different computer codes to study the time-dependent
  hydrodynamics of circumstellar gas/dust shells of AGB stars in their
  final stages of evolution. A two-component radiation hydrodynamics
  code is designed to model a stellar wind driven by radiation pressure
  on dust grains. Combined with detailed stellar evolution calculations,
  this approach allows us to simulate the dynamical response of the AGB
  wind envelope and the emergent spectral energy distribution to temporal
  changes of the stellar luminosity and mass loss rate. A completely
  independent one-component, Godunov-type hydrodynamics code, which is
  particularly well suited to resolve shock fronts, is used to check
  the results obtained with the numerically more diffusive two-component
  code. First, we verify that a presumed short episode of high mass loss
  translates into a correspondingly narrow, high-density shell moving
  through the circumstellar envelope, provided that the mass loss rate,
  and hence the outflow velocity, is essentially constant during the
  mass ejection. In principle, this scenario remains a viable explanation
  for the existence of the very thin molecular shells recently detected
  around some carbon-rich AGB stars. Second, we discovered that an
  alternative mechanism producing very thin shells of greatly enhanced
  gas density can operate in the dusty outflows from AGB stars: the
  interaction of a faster inner wind running into a slower outer wind,
  sweeping up matter at the interface between both type of winds. Based
  on different numerical simulations and on a simple analytical model,
  we show that this mechanism easily leads to the formation of very
  thin shells without the need to invoke large variations of the mass
  loss rate on very short time scales. Finally, we demonstrate that a
  typical helium-shell flash induces both a mass loss `eruption' and a
  two-wind interaction due to the increased outflow velocity during the
  high mass loss phase, leading to the formation of a thin compressed
  gas shell. Very likely, this mechanism is responsible for the origin of
  the CO shells found around some semiregular, optically visible carbon
  stars, the most prominent example being TT Cygni.

---------------------------------------------------------
Title: 2D Numerical Simulation of Stellar Convection
Authors: Steffen, Matthias
2000astro.ph..3074S    Altcode:
  The dynamics and thermal structure of the surface layers of stars
  with outer convection zones can be studied in some detail by means of
  numerical simulations of time-dependent compressible convection. In an
  effort to investigate the properties of “stellar granulation” as a
  function of spectral type, we have carried out elaborate 2-dimensional
  radiation hydrodynamics calculations of surface convection for a variety
  of stellar parameters. The main features of these simulations are
  reviewed, with particular reference to standard mixing length models.

---------------------------------------------------------
Title: A hydrodynamical study of multiple-shell planetaries . I. NGC
    2438
Authors: Corradi, R. L. M.; Schönberner, D.; Steffen, M.; Perinotto,
   M.
2000A&A...354.1071C    Altcode:
  We obtained deep imaging and high-resolution spectroscopy of the
  planetary nebula <ASTROBJ>NGC 2438</ASTROBJ>. In addition to the
  bright inner rim and the faint halo-like shell already known from
  previous imagery, our observations also highlight the existence of
  an even fainter large halo of nearly spherical shape. Analysis of
  the surface-brightness profiles and the line splitting indicates
  a clear ionization stratification within the bright rim, with the
  flow velocities increasing with distance from the central star,
  reaching 37 km s<SUP>-1</SUP>. We compared the surface-brightness
  profiles and kinematical data of <ASTROBJ>NGC 2438</ASTROBJ> with
  state-of-the-art radiation-hydrodynamics models, and obtained a
  surprisingly good qualitative agreement. By means of this modelling
  we show that the faint, halo-like shell has formed by recombination
  from a once well-developed photoionized shell in response to a
  fast luminosity drop of the central star. The large, very faint
  halo is interpreted as being the relic of the now fully ionized AGB
  wind. Also the velocity/ionization stratification and the thickness of
  the bright rim are fully consistent with the prediction of the models
  for such an evolved planetary nebula. The properties of <ASTROBJ>NGC
  2438</ASTROBJ> can be explained by assuming that the planetary nebula
  formation started about 45 000 years after a thermal pulse on the AGB,
  and that the remnant star continued to burn hydrogen in a shell until
  burning has stopped quite recently. Based on observations obtained at
  the 3.5m~NTT telescope of the European Southern Observatory

---------------------------------------------------------
Title: On Carbon Star Evolution in the IRAS Two-Color Diagram
Authors: Szczerba, Ryszard; Steffen, Matthias; Volk, Kevin
2000IAUS..177..581S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Effects of Photospheric Temperature Inhomogeneities on Lithium
    abundance Determinations (2D) (Invited Paper)
Authors: Cayrel, R.; Steffen, M.
2000IAUS..198..437C    Altcode: 2000astro.ph..3075C
  Based on detailed 2D radiation hydrodynamics (RHD) simulations, we have
  investigated the effects of photospheric temperature inhomogeneities
  induced by convection on spectroscopic determinations of the lithium
  abundance. Computations have been performed both for the solar case
  and for a metal-poor dwarf. NLTE effects are taken into account,
  using a five-level atomic model for LiI. Comparisons are presented
  with traditional 1D models having the same effective temperature and
  gravity. The net result is that, while LTE results differ dramatically
  between 1D and 2D models, especially in the metal-poor case, this
  does not remain true when NLTE effects are included: 1D/2D differences
  in the inferred NLTE Li abundance are always well below 0.1 dex. The
  present computations still assume LTE in the continuum. New computations
  removing this assumption are planned for the near future.

---------------------------------------------------------
Title: Radiation Hydrodynamics Simulations of the Solar Chromosphere
Authors: Wedemeyer, Sven; Freytag, Bernd; Steffen, Matthias; Holweger,
   Hartmut
2000AGM....17..P01W    Altcode:
  While heating of the solar corona is commonly attributed to
  reconnection of magnetic field lines, the mechanism responsible for
  heating the chromosphere of the quiet Sun, away from active regions,
  is still under debate<SUP>1,2</SUP>. The basic question which we will
  address in this contribution i s: Can generation of acoustic waves by
  turbulent convection in photospheric and subphotospheric layers explain
  the chromospheric emission of the quiet Sun? With a new 3D radiation
  hydrodynamics code<SUP>3</SUP> we are able to compute models ex tending
  from the upper convection zone to the middle chromosphere. The code
  can handle shocks with a minimum of numerical dissipation. Therefore
  generation and propagation of acoustic waves can be investigated,
  permitting the evaluation of wave dissipation in the chromosphere in
  a physically consistent manner. We present first results and discuss
  the principal problems and future prospects.

---------------------------------------------------------
Title: On the Transition from AGB Stars to Planetaries: The Spherical
    Case
Authors: Schönberner, Detlef; Steffen, Matthias
2000ASPC..199...59S    Altcode: 2000apn..conf...59S; 1999astro.ph.12357S
  We discuss the basic physical model and the relevant processes
  responsible for creating and shaping planetary nebulae out of a cool AGB
  wind envelope. We show that a hydrodynamical treatment along the upper
  AGB leads quite naturally to more realistic starting configurations
  for planetaries with density slopes steeper than r<SUP>-2</SUP>. Taking
  into account photoionization and wind interaction in a realistic manner,
  the hydrodynamics of post-AGB wind envelopes leads to density structures
  and velocity fields in close resemblance to observations of spherical
  or elliptical planetary nebulae.

---------------------------------------------------------
Title: Determination of habitable zones in extrasolar planetary
systems: Where are Gaia's sisters?
Authors: Franck, Siegfried; von Bloh, Werner; Bounama, Christine;
   Steffen, Matthias; Schönberner, Detlef; Schellnhuber, Hans-Joachim
2000JGR...105.1651F    Altcode:
  A general modeling scheme for assessing the suitability for
  life of extrasolar planets is presented. The scheme focuses on
  the identification of the “habitable zone” in main sequence star
  planetary systems accommodating Earth-like components. Our definition of
  habitability is based on the long-term possibility of photosynthetic
  biomass production under geodynamic conditions. Therefore all the
  pertinent astrophysical, climatological, biogeochemical, and geodynamic
  processes involved in the generation of photosynthesis-driven life
  conditions are taken into account. Implicitly, a cogenetic origin of
  the central star and the orbiting planet is assumed. A geostatic model
  version is developed and investigated in parallel for demonstration
  purposes. The numerical solution of the advanced geodynamic model yields
  realistic lookup diagrams for convenient habitability determination. As
  an illustration, the MACHO-98-BLG-35 event is scrutinized. It is shown
  that this event is definitely not tantamount to the discovery of one
  of Gaia's sisters.

---------------------------------------------------------
Title: Carbon- and Oxygen-Rich Stars in the IRAS Two-Color Diagram:
    Results from Hydrodynamical Models of AGB Winds
Authors: Steffen, M.; Szczerba, R.; Men'shchikov, A.; Schönberner, D.
2000IAUS..177..579S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: From the Tip of the AGB Towards a Planetary: A Hydrodynamical
    Simulation
Authors: Schönberner, D.; Steffen, M.; Stahlberg, J.; Kifonidis,
   K.; Blöcker, T.
2000IAUS..177..469S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: The Solar p-Mode Background: Observations and Hydrodynamical
    Models
Authors: Straus, Th.; Steffen, M.; Severino, G.; Freytag, B.
1999ESASP.448..203S    Altcode: 1999mfsp.conf..203S; 1999ESPM....9..203S
  No abstract at ADS

---------------------------------------------------------
Title: A calibration of the mixing-length for solar-type stars based
    on hydrodynamical simulations. I. Methodical aspects and results
    for solar metallicity
Authors: Ludwig, Hans-Günter; Freytag, Bernd; Steffen, Matthias
1999A&A...346..111L    Altcode: 1998astro.ph.11179L
  Based on detailed 2D numerical radiation hydrodynamics (RHD)
  calculations of time-dependent compressible convection, we have
  studied the dynamics and thermal structure of the convective surface
  layers of solar-type stars. The RHD models provide information about
  the convective efficiency in the superadiabatic region at the top of
  convective envelopes and predict the asymptotic value of the entropy of
  the deep, adiabatically stratified layers (Fig. \ref{f:sstarhd}). This
  information is translated into an effective mixing-length parameter
  \alpha<SUB>MLT</SUB> suitable to construct standard stellar
  structure models. We validate the approach by a detailed comparison
  to helioseismic data. The grid of RHD models for solar metallicity
  comprises 58 simulation runs with a helium abundance of Y=0.28 in the
  range of effective temperatures 4300pun {K}&lt;=T<SUB>eff</SUB>&lt;=
  7100pun {K} and gravities 2.54&lt;={log g}&lt;= 4.74. We find a
  moderate, nevertheless significant variation of \alpha<SUB>MLT</SUB>
  between about 1.3 for F-dwarfs and 1.75 for K-subgiants with a
  dominant dependence on T<SUB>eff</SUB> (Fig. \ref{f:mlp}). In the close
  neighbourhood of the Sun we find a plateau where \alpha<SUB>MLT</SUB>
  remains almost constant. The internal accuracy of the calibration
  of \alpha<SUB>MLT</SUB> is estimated to be +/- 0.05 with a possible
  systematic bias towards lower values. An analogous calibration of
  the convection theory of Canuto &amp;\ Mazzitelli (1991, 1992; CMT)
  gives a different temperature dependence but a similar variation of
  the free parameter (Fig. \ref{f:mlpcm}). For the first time, values
  for the gravity-darkening exponent beta are derived independently of
  mixing-length theory: beta = 0.07... 0.10. We show that our findings
  are consistent with constraints from stellar stability considerations
  and provide compact fitting formulae for the calibrations.

---------------------------------------------------------
Title: Long-term evolution of AGB wind envelopes: Insights from
    hydrodynamical models
Authors: Steffen, M.; Schönberner, D.; Szczerba, R.
1999IAUS..191..379S    Altcode:
  Up to now, hydrodynamical models of dust-driven AGB winds do not
  generally take into account the `long-term' changes of the stellar
  parameters (on stellar evolution time scales of 10<SUP>3</SUP> to
  10<SUP>5</SUP> yrs), although it is well known that the luminosity and
  (very likely) the mass loss rate undergo significant variations when
  so called `thermal pulses' occur on the upper AGB. In this review we
  demonstrate that time-dependent radiation hydrodynamics calculations
  are needed to understand the formation, structure, and spectral energy
  distribution of detached dust shells detected by IRAS and ISO. Combined
  with appropriate models, these observations can reveal part of the
  previous mass loss history on the AGB and allow an empirical check of
  presently adopted mass loss laws. Based on insights from hydrodynamical
  simulations, we discuss the two competing scenarios that have been put
  forward to explain the origin of the very thin molecular shells recently
  discovered around some carbon stars. We find that the signature of
  a short mass loss `eruption' broadens quickly with time due to the
  related velocity gradient across the shell. Hence, this scenario is
  not considered a likely explanation of detached CO shells. On the
  other hand, the alternative mechanism, interaction of winds, is shown
  to be capable of producing very thin shells of greatly enhanced gas
  density in the dusty outflows from AGB stars by sweeping up matter at
  the interface between both type of winds.

---------------------------------------------------------
Title: A Calibration of the Mixing-Length for Solar-Type Stars Based
    on Hydrodynamical Models of Stellar Surface Convection
Authors: Freytag, B.; Ludwig, H. -G.; Steffen, M.
1999ASPC..173..225F    Altcode: 1999sstt.conf..225F
  No abstract at ADS

---------------------------------------------------------
Title: On the origin of thin detached gas shells around AGB stars:
    Insights from time-dependent hydrodynamical simulations
Authors: Steffen, Matthias; Schönberner, Detlef
1999AGAb...15..109S    Altcode:
  We have applied two different computer codes to study the time-dependent
  hydrodynamics of circumstellar gas/dust shells of AGB stars in their
  final stages of evolution. We verify that a presumed short episode of
  high mass loss translates into a correspondingly narrow, high-density
  shell moving through the circumstellar envelope at supersonic speed,
  provided that the mass loss rate, and hence the outflow velocity, is
  essentially constant during the mass loss `eruption'. In principle,
  this scenario remains a viable explanation for the existence of the
  very thin molecular shells recently detected around some carbon-rich AGB
  stars. We discovered that an alternative mechanism producing very thin
  shells of greatly enhanced gas density can operate in the dusty outflows
  from carbon-rich AGB stars: the interaction of a faster inner wind
  running into a slower outer wind, sweeping up matter at the interface
  between both type of winds. We show that this mechanism easily leads
  to the formation of very thin shells without the need to invoke large
  variations of the mass loss rate on very short time scales. Finally,
  we demonstrate that a typical He-shell flash produces both a mass loss
  `eruption' and a two-wind interaction due to the increased outflow
  velocity during the high mass loss phase, leading to the formation
  of a thin compressed gas shell. We propose that this mechanism is
  responsible for the origin of the observed very thin CO shell around
  the optically visible carbon star TT Cygni.

---------------------------------------------------------
Title: Silicon as a cosmic reference element: a reassessment of the
    solar SI abundance
Authors: Wedemeyer, Sven; Holweger, Hartmut; Steffen, Matthias
1999AGAb...15..113V    Altcode: 1999AGM....15..P53V; 1999AGM....15..P54W
  Silicon is an important reference elements for comparing various
  types of cosmic matter with the Sun. The most widely used sources
  of solar (photospheric) abundances, the compilation by Anders &amp;
  Grevesse (1989) and its updates (e.g. Grevesse &amp; Sauval 1998), are
  based on standard abundance analyses employing 1D solar models and,
  in most cases, assuming LTE. We report NLTE calculations for Si and
  a first attempt to determine the effect of horizontal temperature
  inhomogeneities associated with convection on the photospheric
  abundance of Si. We combine the result with that obtained previously
  for O and Fe (Aellig et al. 1999; Schnabel et al. 1999) and compare
  the photospheric Si/Fe, Si/O and Si/H abundance ratios with literature
  data for meteorites, the corona and solar wind, energetic particles and
  galactic B stars and H ii regions. References: Aellig M.R., Holweger H.,
  Bochsler P., et al., 1999, Solar Wind Nine, AIP Conf. Proc. Vol. 471,
  255 Anders E., Grevesse N., 1989, Geochim. Comochim. Acta 53, 197
  Grevesse N., Sauval A.J., 1998, Space Sci. Rev. 85, 161 Schnabel R.,
  Kock M., Holweger H., 1999, A&amp;A 342, 610

---------------------------------------------------------
Title: Line Formation in Convective Stellar Atmospheres
Authors: Steffen, Matthias; Holweger, Hartmut
1999AGb....15..107S    Altcode: 1999AGM....15..P40S
  Convection affects the temperature structure of a stellar atmosphere
  in a twofold way: it influences the mean vertical stratification and
  introduces horizontal inhomogeneities. This poses several questions: (i)
  What is the “right” alpha_MLT to produce the correct mean temperature
  stratification in the framework of mixing-length theory ? (ii) What
  errors are introduced, in the context of spectroscopic abundance
  determinations, by representing the horizontally averaged spectrum
  of an inhomogeneous atmosphere by the spectrum of a plane-parallel
  mean stratification? (iii) Is there something like a spectroscopically
  equivalent mean stratification of an inhomogeneous atmosphere? In order
  to address these questions, we have computed synthetic line profiles for
  a sample of fictitious spectral lines of different chemical elements,
  based on both mixing-length atmospheres and 2D hydrodynamical solar
  granulation models. Through a differential comparison of the equivalent
  widths computed from the inhomogeneous atmospheres and different 1D
  mean models, respectively, we derive correction factors to be applied
  to standard 1D spectroscopic abundance determinations in order to
  correct for the effects of stellar `granulation'. We find that the
  abundance correction depends sensitively on the ionization stage of
  the chemical element and on the excitation potential of the spectral
  line considered. In some cases the `granulation correction' can amount
  to -0.2 dex.

---------------------------------------------------------
Title: Balmer Line Formation in Convective Stellar Atmospheres
Authors: Steffen, M.; Ludwig, H. -G.
1999ASPC..173..217S    Altcode: 1999sstt.conf..217S
  No abstract at ADS

---------------------------------------------------------
Title: Formation and Evolution of Planetary Nebulae
Authors: Schönberner, D.; Steffen, M.
1999ASPC..188..281S    Altcode: 1999oisc.conf..281S
  No abstract at ADS

---------------------------------------------------------
Title: Hydrodynamical models and synthetic spectra of circumstellar
    dust shells around AGB stars. II. Time-dependent simulations
Authors: Steffen, Matthias; Szczerba, Ryszard; Schoenberner, Detlef
1998A&A...337..149S    Altcode:
  We have employed time-dependent two-component hydrodynamics/radiative
  transfer calculations to investigate the structure, dynamics and
  emergent spectral energy distribution of dusty circumstellar shells
  around carbon and oxygen stars in the final stages of their AGB
  evolution. These internally consistent, physical models describe a
  stellar wind driven by radiation pressure on dust grains and subsequent
  momentum transfer to the gas component via collisions. Detailed stellar
  evolution calculations, with a prescribed mass loss rate that is a
  function of the fundamental stellar parameters, have been used as a
  time-dependent inner boundary condition for the numerical solution
  of the coupled equations of hydrodynamics and frequency-dependent
  radiative transfer governing the structure and temporal evolution of
  the circumstellar dust/gas shell. The calculations are based on one
  particular evolutionary track for an initial stellar mass M_i=3.0
  M<SUB>s</SUB>un\ and a final mass M_f=0.605 M<SUB>s</SUB>un, but for
  different assumptions concerning the composition of the dust grains:
  amorphous carbon or “astronomical” silicates. Using our hydrodynamics
  code to simulate the dynamical response of the circumstellar wind
  shell to the evolutionary changes of the stellar parameters, we
  find that the large temporal variations of stellar luminosity and
  mass loss rate associated with the final thermal pulses near the
  end of the AGB evolution lead to characteristic, time-dependent
  signatures in the density structure and emergent energy distribution
  of the circumstellar dust shell. We present the resulting “loops”
  in the IRAS two-color-diagram, which we find to extend to regions
  quite remote from the simple color-color relation defined by steady
  state models. These time-dependent hydrodynamical models explain the
  existence of carbon and oxygen stars with excess emission near lambda
  60 and 100 mu m as a natural consequence of the sharp decrease of the
  mass loss rate following a thermal pulse, leading to the development
  of a detached dust shell. As an illustration, we present a series
  of synthetic spectra and corresponding 100 mu m surface brightness
  distributions showing the time-evolution of the circumstellar dust
  emission during a thermal pulse cycle, both for a carbon-rich and an
  oxygen-rich dust shell. We demonstrate that it is unrealistic to assume
  a fixed velocity profile which is independent of mass loss rate: to a
  first approximation, the gas velocity is a bimodal function of the mass
  loss rate. A short event of high mass loss does not simply translate
  into a correspondingly narrow, high-density shell moving through
  the circumstellar envelope. Rather, the signature of a short mass
  loss peak broadens due to velocity gradients as it moves towards the
  outer regions of the wind. Hence, this is hardly a viable scenario to
  explain the existence of very thin molecular shells that have recently
  been detected around some carbon stars. Our simulations suggest a more
  promising mechanism producing thin shells of enhanced gas density in
  the outer regions of carbon-rich AGB shells: interaction of winds of
  different speed and density.

---------------------------------------------------------
Title: Lithium Depletion in the Sun: A Study of Mixing Based on
    Hydrodynamical Simulations
Authors: Blöcker, T.; Holweger, H.; Freytag, B.; Herwig, F.; Ludwig,
   H. -G.; Steffen, M.
1998SSRv...85..105B    Altcode: 1998astro.ph..6310B
  Based on radiation hydrodynamics modeling of stellar convection zones,
  a diffusion scheme has been devised describing the downward penetration
  of convective motions beyond the Schwarzschild boundary (overshoot)
  into the radiative interior. This scheme of exponential diffusive
  overshoot has already been successfully applied to AGB stars. Here
  we present an application to the Sun in order to determine the time
  scale and depth extent of this additional mixing, i.e. diffusive
  overshoot at the base of the convective envelope. We calculated the
  associated destruction of lithium during the evolution towards and on
  the main-sequence. We found that the slow-mixing processes induced by
  the diffusive overshoot may lead to a substantial depletion of lithium
  during the Sun's main-sequence evolution.

---------------------------------------------------------
Title: IR-Colors for Models of Post-AGB Evolution
Authors: Szczerba, R.; Steffen, M.
1998Ap&SS.262..187S    Altcode: 1999Ap&SS.262..187S
  No abstract at ADS

---------------------------------------------------------
Title: Lithium Depletion in the Sun: A Study of Mixing Based on
    Hydrodynamical Simulations
Authors: Blöcker, T.; Holweger, H.; Freytag, B.; Herwig, F.; Ludwig,
   H. -G.; Steffen, M.
1998sce..conf..105B    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Hydrodynamical Modelling of the Evolution of Dusty Outflows
    from AGB-Stars
Authors: Schönberner, D.; Steffen, M.; Szczerba, R.
1998Ap&SS.255..459S    Altcode: 1997Ap&SS.255..459S
  No abstract at ADS

---------------------------------------------------------
Title: An improved calibration of the mixing-length based on
    simulations of solar-type convection
Authors: Ludwig, H. -G.; Freytag, B.; Steffen, M.
1998IAUS..185..115L    Altcode:
  Based on detailed 2D numerical radiation hydrodynamics (RHD)
  calculations of time-dependent compressible convection, we have studied
  the dynamics and thermal structure of the convective surface layers
  of stars in the range of effective temperatures and gravities between
  4500 pun{K} &lt;= Teff &lt;= 7100 pun{K} and 2.54 &lt;= logg &lt;=
  4.74. Although our hydrodynamical models describe only the shallow,
  strongly superadiabatic layers at the top of the convective stellar
  envelope, we demonstrate that they provide information about the value
  of the entropy of the deeper, adiabatically stratified regions. This
  quantity can be translated into an effective mixing-length parameter
  suitable for constructing standard stellar structure models. We
  show that a hydrodynamically calibrated envelope model for the Sun
  closely matches the known adiabat and corresponding depth of the solar
  convection zone. We determined the dependence of the mixing-length
  parameter on Teff, log g, and chemical composition obtaining a moderate
  variation over the range studied. We note that the recent description
  of convection by Canuto &amp; Mazzitelli extended by including a
  variable amount of overshoot does not lead to a smaller variation of
  the controlling parameter. We discuss the consistency of our results
  with findings derived in the context of the tentative detection of
  solar-like oscillations in eta Bootis.

---------------------------------------------------------
Title: A calibration of mixing length theory based on RHD simulations
    of solar-type convection
Authors: Ludwig, H. -G.; Freytag, B.; Steffen, M.
1997ASSL..225...59L    Altcode: 1997scor.proc...59L
  Radiation hydrodynamics (RHD) models provide detailed information
  about the dynamics, thermal structure, and convective efficiency
  of the superadiabatic region at the top of solar-type convection
  zones, and allow an extrapolation of the entropy (s*) in their deep,
  adiabatic layers. For the Sun we find a close agreement between s*
  inferred from our RHD models and an empirical determination of s*
  from helioseismology. In the framework of mixing length theory (MLT),
  s* is translated to an effective mixing-length parameter (alpha c)
  appropriate to construct global stellar models. The calibration based
  on our present set of 2D RHD models shows a moderate variation of
  alpha c across the domain of the HRD investigated so far.

---------------------------------------------------------
Title: Hydrodynamical models and synthetic spectra of circumstellar
    dust shells around AGB stars
Authors: Steffen, M.; Szczerba, R.; Men'shchikov, A.; Schoenberner, D.
1997A&AS..126...39S    Altcode:
  We present a sample of hydrodynamical steady state models of
  circumstellar gas/dust shells around late type giants together with
  computed spectral energy distributions (SEDs). In these models,
  the stellar wind is driven by radiation pressure on dust grains and
  subsequent momentum transfer to the gas molecules via collisions. Given
  the fundamental stellar parameters (M_*, L_*, T_eff), the mass loss rate
  (M_dot), and the dust properties, a self-consistent physical model of
  the circumstellar gas/dust shell is obtained from the numerical solution
  of the coupled equations of hydrodynamics and radiative transfer. The
  computed outflow velocities and infrared fluxes of the circumstellar
  envelopes can be compared directly with the observed properties of
  stars on asymptotic giant branch. Plotting the positions of our steady
  state models in different IRAS two-color-diagrams, we confirm that, for
  fixed dust properties, all models fall on a simple color-color relation
  with M_dot (or optical depth) as the only parameter. Surprisingly, we
  find a good agreement between the synthetic spectra resulting from the
  self-consistent hydrodynamical approach and those obtained from much
  simpler models based on a constant outflow velocity and ignoring drift
  of dust relative to the gas. Our models are compared with the results
  of similar calculations by \cite[Netzer &amp; Elitzur (1993).]{Net93}
  We find significant differences which are probably the result of some
  unrealistic approximations in the treatment of radiative transfer
  underlying the model calculations of Netzer &amp; Elitzur. Moreover,
  our results demonstrate that, in general, gas pressure cannot be
  neglected for winds with relatively low expansion velocities (u_e
  &lt; 30 km/s). For given stellar parameters and dust properties, the
  theoretical minimum (maximum) mass loss rate decreases (increases)
  significantly when gas pressure is taken into account.

---------------------------------------------------------
Title: Numerical simulations of stellar surface convection.
Authors: Freytag, B.; Steffen, M.
1997AGAb...13..176F    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Modeling the Long-Term Evolution of Dusty Outflow Outflows
    of AGB-Stars
Authors: Steffen, M.; Szczerba, R.
1997Ap&SS.251..131S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: IR-Colors for Models of Post-AGB Evolution
Authors: Szczerba, R.; Steffen, M.
1997Ap&SS.251..149S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: VizieR Online Data Catalog: Models of circumstellar dust shells
    (Steffen+ 1997)
Authors: Steffen, M.; Szczerba, R.; Men'shchikov, A.; Schoenberner, D.
1997yCat..41260039S    Altcode:
  Main properties of the steady state hydrodynamical models of
  circumstellar gas/dust shells around late type giants, computed for
  different stellar parameters (mass, luminosity, effective temperature)
  and dust composition (astronomical silicates, graphite, or amorphous
  carbon, with properties given in Tab.1 and Fig.1). Each table lists
  the results as a function of the adopted mass loss rate for fixed
  stellar parameters and dust properties. Tables 2 - 11 are related to
  Figures 2 - 11: Each of the figures shows the velocity structure and
  the resulting spectral energy distribution for a subset of models
  listed in the respective table. <P />(2 data files).

---------------------------------------------------------
Title: On the Scale of Photospheric Convection
Authors: Freytag, B.; Holweger, H.; Steffen, M.; Ludwig, H. -G.
1997svlt.work..316F    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Through the upper AGB towards a planetary: a hydrodynamical
    simulation.
Authors: Schönberner, D.; Steffen, M.; Stahlberg, J.; Kifonidis,
   K.; Blöcker, T.
1997seas.conf..146S    Altcode: 1997ase..work..146S
  The authors present an exploratory investigation of the dynamical
  evolution of a dusty stellar wind envelope along the upper AGB and
  its transformation into a planetary nebula. They find the existence
  of AGB stars with detached shells to be a natural consequence of the
  mass loss variations during a thermal pulse. It is also shown that
  due to the large dynamical effects caused by the ionizing radiation
  field and the fast wind of the central star, it is impossible to
  deduce the AGB mass loss history from the planetary's density and
  velocity distribution. The structure of the halo, however, is still
  determined by the AGB mass loss history. The rapid decline of mass
  loss expected in the aftermath of thermal pulses leads to extended
  shells of low densities and explains halos with sharp boundaries. The
  density structure and velocity field of the model planetary closely
  resemble those of observed planetary nebulae.

---------------------------------------------------------
Title: Time-dependent hydrodynamical models of circumstellar dust
    shells around carbon- and oxygen-rich AGB stars.
Authors: Steffen, M.; Szczerba, R.; Men'shchikov, A.; Schönberner, D.
1997seas.conf..154S    Altcode: 1997ase..work..154S
  The authors have employed time-dependent two component hydrodynamics -
  radiative transfer calculations to investigate the structure, dynamics
  and emergent spectral energy distribution of dusty circumstellar
  shells around carbon and oxygen stars in the final stages of their AGB
  evolution. In these models, the wind is driven by radiation pressure on
  dust grains and subsequent momentum transfer to the gas molecules by
  collisions. Detailed stellar evolution calculations with a prescribed
  mass loss rate that varies as a function of the fundamental stellar
  parameters provide the time-dependent inner boundary conditions for
  the numerical solution of the coupled equations of hydrodynamics and
  radiative transfer which describe a consistent physical model of the
  evolution of the circumstellar shell. Using the hydrodynamical code
  to simulate the dynamical response of the circumstellar wind shell
  to the evolutionary changes of the stellar parameters, the authors
  find that the large temporal variations of L and M˙ associated with
  the final thermal pulses near the end of the AGB evolution lead to
  characteristic, time-dependent signatures in the density structure
  and in the infrared emission of the circumstellar dust.

---------------------------------------------------------
Title: Through the AGB towards a Planetary: A hydrodynamical
    simulation
Authors: Steffen, M.; Schonberner, D.; Kifonidis, K.; Stahlberg, J.
1997IAUS..180..368S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Hydrodynamical models of stellar convection. The role of
    overshoot in DA white dwarfs, A-type stars, and the Sun.
Authors: Freytag, B.; Ludwig, H. -G.; Steffen, M.
1996A&A...313..497F    Altcode:
  Based on two-dimensional numerical radiation hydrodynamics
  simulations of time-dependent compressible convection, we have
  studied the structure and dynamics of a variety of shallow stellar
  surface convection zones. Our present grid of models includes
  detailed simulations of surface convection in solar-type stars,
  main-sequence A-type stars and cool DA white dwarfs, as well as
  numerical experiments to study convection and overshoot at the base of
  the solar convection zone. Taking into account a realistic equation of
  state (including the effects of ionization) and adopting an elaborate
  treatment of non-local radiative transfer (with appropriate grey
  or frequency-dependent opacities), our simulations are designed to
  represent specific stellar objects characterized by T_eff_, logg, and
  chemical composition. Contrary to solar-type stars, the A-type stars and
  cool DA white dwarfs investigated here have shallow convection zones
  which fit into the computational domain together with thick stable
  buffer layers on top and below, thus permitting a study of convective
  overshoot under genuine conditions. We find that convective motions
  extend well beyond the boundary of the convectively unstable region,
  with vertical velocities decaying exponentially with depth in the
  deeper parts of the lower overshoot region, as expected for linear
  g^-^-modes. Even though convective velocities are reduced by orders of
  magnitude, they are still able to counteract molecular diffusion. For
  a quantitative description of convective mixing in the far overshoot
  layers we have derived a depth dependent diffusion coefficient from
  the numerical simulations. In combination with otherwise independent
  1D diffusion calculations for a trace element, this allows the
  determination of the "effective depth" of the overshoot region. For
  a typical main-sequence A-type star (T_eff_=7943#1, logg=4.34) the
  mass in the overshoot region exceeds the mass in the unstable region
  by approximately a factor 10. The amount of overshoot in cool DA white
  dwarfs (around T_eff_=12200#1) is even larger: the convectively mixed
  mass is increased by roughly a factor 100.

---------------------------------------------------------
Title: On the detection of shocks in the solar granulation.
Authors: Solanki, S. K.; Rueedi, I.; Bianda, M.; Steffen, M.
1996A&A...308..623S    Altcode:
  We investigate the spectral signature of a hydrodynamic simulation of
  solar granulation and compare it with high resolution observations. The
  model gives the correct qualitative trend of increasing line width
  with decreasing continuum intensity seen by Nesis et al. (1992)
  and interpreted by them as a sign of post-shock turbulence. We find,
  however, that the profiles in the dark downflow lanes are broader even
  when there is no horizontal transonic flow or shock in the vicinity. We
  conclude that the observations of Nesis et al. do not provide any firm
  evidence for the presence of granular transonic flows. Nevertheless,
  the simulation predicts a promising diagnostic of shocked horizontal
  flows. We find that at the locations of the shocks the line profiles
  are particularly broad, especially near the solar limb. We present
  observations of quiet solar regions that show this specific signature
  of shocks and thus support the theoretical prediction of transonic
  granular flows.

---------------------------------------------------------
Title: Lyapunov exponents for solar surface convection.
Authors: Steffen, M.; Freytag, B.
1995CSF.....5.1965S    Altcode:
  The authors have carried out detailed 2D numerical radiation
  hydrodynamics calculations, specifically designed to model
  time-dependent, compressible convection in the surface layers of the
  Sun. These simulations, which take into account a realistic equation
  of state and use an elaborate scheme to describe multi-dimensional,
  non-local, frequency-dependent radiative transfer, allow a direct
  comparison with observed photometric and spectroscopic properties of
  solar granulation. Their purpose is to enhance the understanding of
  the dynamics and thermal structure of convective stellar atmospheres,
  and to investigate the generation of acoustic energy by turbulent
  convection. The authors briefly present some of the main properties of
  their solar convection models. In particular, the authors demonstrate
  the chaotic behaviour of solar surface convection, estimating the
  magnitude of the two largest Lyapunov exponents, λ<SUB>1</SUB> and
  λ<SUB>2</SUB>, by analysing the time evolution of three simulations
  with slightly different initial conditions. The authors find that
  both λ<SUB>1</SUB> and λ<SUB>2</SUB> are positive and of similar
  magnitude as expected for a chaotic system of high dimension. The
  corresponding characteristic time scale λ<SUB>1</SUB><SUP>-1</SUP>
  of approximately 320 s is comparable to the convective turnover time.

---------------------------------------------------------
Title: Synthetic spectra computed from hydrodynamical model
    atmospheres of DA white dwarfs.
Authors: Steffen, M.; Ludwig, H. -G.; Freytag, B.
1995A&A...300..473S    Altcode:
  From detailed 2-dimensional numerical radiation hydrodynamics
  calculations of time-dependent compressible convection we have obtained
  the thermal structure of the convective surface layers of DA white
  dwarfs with effective temperatures near the blue edge of the ZZ Ceti
  instability strip. Synthetic line profiles of H<SUB>beta</SUB>_ and the
  red wing of L<SUB>alpha</SUB>_ (including the very temperature sensitive
  satellite absorption features) computed from two representative
  inhomogeneous hydrodynamical models (T_eff_=12200K, 12600K; log g=8.0)
  are compared with the spectra resulting from different plane-parallel
  model atmospheres. We find that it is possible to represent a given
  inhomogeneous atmosphere by a spectroscopically equivalent 1D model,
  constructed to have the same frequency-integrated radiative flux as
  the respective 2D hydrodynamical model at all depths. Synthetic spectra
  computed from this representative 1D model are almost indistinguishable
  from the horizontally averaged 2D synthetic spectra of the corresponding
  inhomogeneous model. We conclude that in the investigated range of
  effective temperature (probably even for the whole range of convective
  DAs), spectroscopic analysis based on appropriate 1D atmospheres is
  almost unaffected by systematic errors associated with non-linear flux
  variations due to the substantial thermal inhomogeneities generated
  by photospheric convection in these stars. This work provides the
  basis for a well defined comparison between 2D or 3D hydrodynamical
  convection models and 1D standard mixing length models.

---------------------------------------------------------
Title: Hydrodynamical model atmospheres: convection and line formation
    in the Sun
Authors: Ludwig, H. -G.; Steffen, M.
1995IAUS..176P.235L    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: The Mixing-Length Parameter for Solar-Type Convection Zones
    Inferred from Hydrodynamical Models of the Surface Layers
Authors: Ludwig, H. -G.; Freytag, B.; Steffen, M.; Wagenhuber, J.
1995LIACo..32..213L    Altcode: 1995sews.book..213L
  No abstract at ADS

---------------------------------------------------------
Title: Numerical Simulations of Convection and Overshoot in the
    Envelope of DA White Dwarfs
Authors: Freytag, Bernd; Steffen, Matthias; Ludwig, Hans-Günter
1995LNP...443...88F    Altcode: 1995whdw.conf...88F
  We present results of realistic 21) numerical radiation hydrodynamics
  calculations, simulating the surface convection zones of DA white
  dwarfs in the range of effective temperatures from 14 200 K down
  to 11400 K. Comparison with mixing length theory (MLT) yields a
  conflicting picture: The dynamics of convection is not governed by
  up- and downflowing bubbles which dissolve after travelling some
  characteristic distance - but by the formation, advection, merging,
  and disruption of fast narrow downdrafts in a slowly upstreaming
  surrounding. MLT tremendously underestimates the depth of the region
  where material is mixed. Nevertheless, it turns out that a mixing
  length model with α = 1.5 gives a good fit of the photospheric
  temperature structure (T <SUB>eff</SUB> = 12 600 K) and that a 1D
  temperature stratification suffices to reproduce the mean spectrum
  of the 2D simulations, indicating that the photospheric temperature
  inhomogeneities are negligible for spectroscopic analysis. In deeper
  layers the temperature stratification of our hydrodynamical models
  corresponds to larger values of α. Introducing our envelope models into
  nonadiabatic pulsation calculations results in a blue edge of the ZZ
  Ceti instability strip near T <SUB>eff</SUB> = 12 400 K at log g = 8.0.

---------------------------------------------------------
Title: Spectroscopic Effects of T-Inhomogeneities in the Atmospheres
    of DA White Dwarfs
Authors: Ludwig, Hans-Günter; Steffen, Matthias
1995LNP...443..128L    Altcode: 1995whdw.conf..128L
  No abstract at ADS

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Title: Numerical simulations of surface convection in solar-type stars
Authors: Freytag, B.; Steffen, M.
1995IAUS..176P.111F    Altcode:
  No abstract at ADS

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Title: Numerical simulations of convection at the surface of a ZZ
    Ceti white dwarf.
Authors: Ludwig, H. -G.; Jordan, S.; Steffen, M.
1994A&A...284..105L    Altcode:
  We applied two-dimensional hydrodynamics and non-grey radiative transfer
  calculations to the surface layers of a hydrogen-rich white dwarf
  (spectral type DA) with T_eff_=12600K and log(g)=8.0, corresponding to
  a position in the HR-diagram slightly cooler than the hot boundary of
  the ZZ Ceti instability strip. In our simulations the entire convection
  zone including the overshoot layers is embedded in the computational box
  so that we obtain a complete and detailed model of convection for this
  representative object. We address the important question to what extent
  models based on mixing length theory (MLT) are able to predict the
  physical properties of convection. We find a rapidly (timescale ~100ms)
  evolving flow pattern with fast concentrated downdrafts surrounded by
  slow broad upflows of warmer material. Convection carries up to 30%
  of the total flux and excites internal gravity waves by dynamical
  processes associated with the merging of downdrafts. The mean entropy
  gradient is reversed with respect to MLT predictions in the deeper
  layers of the convection zone. Strong overshoot occurs at its upper
  and lower boundary. A synthetic spectrum calculated from the mean
  photospheric temperature stratification can be fitted satisfactorily
  with a MLT model adopting α=1.5. At greater depth the temperature
  profile approaches a model with α=4. The total depth of the convective
  layers is rather small compared to values suggested by studies of the
  excitation mechanism for the pulsations of DAs.

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Title: Acoustic flux generation in the solar convection zone
Authors: Steffen, M.
1994smf..conf..294S    Altcode:
  No abstract at ADS

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Title: Shocks in the solar photosphere and their spectroscopic
    signature
Authors: Steffen, M.; Freytag, B.; Holweger, H.
1994smf..conf..298S    Altcode:
  No abstract at ADS

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Title: Numerical simulations of convection at the surface of a ZZ
    Ceti white dwarf.
Authors: Ludwig, H. -G.; Jordan, S.; Steffen, M.
1993AGAb....9..147L    Altcode:
  No abstract at ADS

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Title: Acoustic flux generation in the solar convection zone.
Authors: Steffen, M.
1993AGAb....9..118S    Altcode:
  No abstract at ADS

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Title: The Depth of the Solar Convection Zone Inferred from
    Hydrodynamical Models of the Surface Layers
Authors: Steffen, M.
1993ASPC...40..300S    Altcode: 1993ist..proc..300S
  No abstract at ADS

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Title: First numerical simulations of convection at the surface of
    a ZZ Ceti white dwarf
Authors: Ludwig, H. -G.; Jordan, S.; Steffen, M.
1993ASIC..403..471L    Altcode: 1993wdao.conf..471L
  No abstract at ADS