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Modeling stopping power of ions in plasmas using parametric potentials
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作者 Tanguy Barges Delattre Sébastien Rassou Jean-Christophe Pain 《Matter and Radiation at Extremes》 2025年第6期86-100,共15页
We present a study of the ion stopping power due to free and bound electrons in a warm dense plasma.Our main goal is to propose a method of stopping-power calculation expected to be valid for any ionization degree.The... We present a study of the ion stopping power due to free and bound electrons in a warm dense plasma.Our main goal is to propose a method of stopping-power calculation expected to be valid for any ionization degree.The free-electron contribution is described by the Maynard–Deutsch–Zimmerman formula,and the bound-electron contribution relies on the Bethe formula with corrections,in particular taking into account density and shell effects.The results of the bound-state computation using three different parametric potentials are investigated within the Garbet formalism for the mean excitation energy.The first parametric potential is due to Green,Sellin,and Zachor,the second one was proposed by Yunta,and the third one was introduced by Klapisch in the framework of atomic-structure computations.The results are compared with those of self-consistent average-atom calculations.This approach correctly bridges the limits of neutral and fully ionized matter. 展开更多
关键词 warm dense plasmaour free bound electrons maynard deutsch zimmerman formulaand parametric potentials ion stopping power bethe formula free electrons bound electrons
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Erratum and Addendum:Improvement of nuclear semi-empirical mass formula by including shell effect(Chin.Phys.C,49(11):114103(2025))
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作者 Qing Wu Wei-Feng Li +2 位作者 Zhong-Ming Niu Hao-Zhao Liang Min Shi 《Chinese Physics C》 2025年第12期448-448,共1页
This paper was published online on 28 June 2025,and there is a numerical error in Fig.1 of the published version.This correction only resulted in minor changes to the last decimal places of the root mean square(rms)de... This paper was published online on 28 June 2025,and there is a numerical error in Fig.1 of the published version.This correction only resulted in minor changes to the last decimal places of the root mean square(rms)deviation of the BWK formula,and through rigorous verification,such discrepancies will not have any impact on the key conclusions of the paper.The Fig.1 in the published version is corrected as Fig.1 in this erratum.Fig.1.Differences between the experimental binding energies and predictions calculated using the BWK*and BWK formulas,respectively.The dashed lines denote the traditional magic numbers. 展开更多
关键词 erratum bwk formulaand nuclear semi empirical mass formula root mean square deviation rigorous verificationsuch shell effect ADDENDUM experimental binding energies
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