2019
DOI: 10.1016/j.hedp.2019.01.003
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Plasma opacity calculations using the Starrett and Saumon average-atom model with ion correlations

Abstract: We present the opacities of iron, aluminum, and bromine plasmas calculated using the Starrett and Saumon average-atom model allowing for ion correlations. We show that the use of earlier average-atom ion-correlation model of Rozsnyai, as has recently been done in the solar opacity calculations, overestimates the effect of ion correlations on plasma opacities.The reason for this overestimation is discussed.

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Cited by 11 publications
(6 citation statements)
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References 62 publications
(127 reference statements)
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“…Regarding plasma embedding effects in the solar interior, Krief et al (2018) have used the ion-ion correlation model of Rozsnyai (1991Rozsnyai ( , 1992 to re-evaluate the Fe Rosseland mean opacity in conditions similar to the base of the convection zone and have found a 15% increase. However, a more recent calculation (Ovechkin et al 2019) based on the Starrett-Saumon average-atom model has questioned this result as an overestimate due to a limited treatment of the ion-ion repulsion, which is one of the points we have emphasized in the present work.…”
Section: Astrophysical Implicationsmentioning
confidence: 77%
“…Regarding plasma embedding effects in the solar interior, Krief et al (2018) have used the ion-ion correlation model of Rozsnyai (1991Rozsnyai ( , 1992 to re-evaluate the Fe Rosseland mean opacity in conditions similar to the base of the convection zone and have found a 15% increase. However, a more recent calculation (Ovechkin et al 2019) based on the Starrett-Saumon average-atom model has questioned this result as an overestimate due to a limited treatment of the ion-ion repulsion, which is one of the points we have emphasized in the present work.…”
Section: Astrophysical Implicationsmentioning
confidence: 77%
“…Detailed finite temperature density functional theory (DFT) calculations in the spherical average atom approximation [33,[37][38][39][40][41][42][43][44][45] followed by STA calculations using the atomic code STAR [28,29], were performed over a wide range of plasma temperatures: 100eV-10keV and densities: 10 −3 − 10 3 g/cm 3 , for the following low, mid and high Z elements -Silicone (Z=14), Iron (Z=26), Xenon (Z=54) and Gold (Z=79). The results are shown in Figs 5-8, and include the average ionization, the chem-ical potential, the number of bound shells, the combinatoric number of configurations over all ionization levels (eq.…”
Section: Resultsmentioning
confidence: 99%
“…where A is the set of all shells from which configurations are constructed. We note that, in general, the number of bound shells is a function of the atomic number, temperature and density, which determines the self consistent central potential -for example, a higher Z element has a larger number of bound shells, due to the higher nucleus charge and a higher density plasma may have a smaller number of shells due to an increased pressure ionization effect (bound states dissolving into the continuum [33,[37][38][39][40][41][42][43][44][45]).…”
Section: Combinatoric Number Of Configurationsmentioning
confidence: 99%
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“…To investigate the effect of ion correlations on plasma opacities, Ovechkin et al performed opacity calculations using an ion-correlation average-atom model, following the recent Starrett and Saumon formulation [58,59]. The model was implemented in the RE-SEOS code [60][61][62] that implements a generalized version of the STA approach providing a substantial acceleration of the photo-absorption and photo-ionization calculations with almost the same accuracy as that one obtained with the original superconfiguration approach. As a result, RESEOS predicts a much smaller increase of the Rosseland mean opacity due to ionic correlations (5.5%) than the above mentioned STAR code does (20%).…”
Section: The Reseos Code By Ovechkin Et Almentioning
confidence: 99%