首页> 外文期刊>Journal of Physics, B. Atomic, Molecular and Optical Physics: An Institute of Physics Journal >Double ionization of heavy positive ions by electron impact: empirical formula and fitting parameters for ionization cross sections
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Double ionization of heavy positive ions by electron impact: empirical formula and fitting parameters for ionization cross sections

机译:重正离子通过电子碰撞的双重电离:电离截面的经验公式和拟合参数

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Electron-impact double-ionization processes of multi-electron heavy ions from Ti up to Bi (nuclear charge from Z = 22 up to Z = 83) are investigated for incident electron energies E < 50 I-th where I-th is the threshold energy for double ionization. The following ions are considered: Tiq+ (q = 1-6), Feq+ (q = 1, 3-6), Niq+ (q = 1-6), Gaq+ (q = 1-6), Krq+ (q = 1-4), Moq+ (q = 1-6), Prq+ (q = 1-4), Smq+ (q = 1-6), Wq+ (q = 1-6), Pbq+ (q = 1-9) and Biq+ (q = 1-10, 12). On the basis of experimental data, mostly obtained at an electron-ion crossed-beams set-up in Giessen, and quantum-mechanical considerations, a simple semi-empirical formula with six fitting parameters is developed taking into account the contribution of direct double ionization of two outer-shell electrons of the ions and also of single inner-shell ionization processes followed by autoionization with additional ejection of an electron as was suggested in our previous paper (Shevelko et al 2005). The formula obtained there was found to describe well the available experimental double-ionization cross sections within an accuracy of 20-30%. However, for multielectron, very heavy ions significant deviations of that formula from experiment are found in the low-energy region. These deviations are most likely caused by higher order processes, including inner-shell excitation and subsequent double autoionization (EDA). The tabulated parameters can be used for easy analytical representation of the double-ionization cross sections of heavy positive ions in the modelling of laboratory and astrophysical plasmas.
机译:研究了从Ti到Bi的多电子重离子的电子碰撞双电离过程(从Z = 22到Z = 83的核电荷)对入射电子能量E <50 I-th的影响,其中I-th是阈值双电离的能量。考虑以下离子:Tiq +(q = 1-6),Feq +(q = 1,3-6),Niq +(q = 1-6),Gaq +(q = 1-6),Krq +(q = 1- 4),Moq +(q = 1-6),Prq +(q = 1-4),Smq +(q = 1-6),Wq +(q = 1-6),Pbq +(q = 1-9)和Biq +( q = 1-10,12)。根据主要在吉森(Giessen)设置的电子离子交叉电子束获得的实验数据,以及量子力学的考虑,考虑到直接双电离的作用,建立了具有六个拟合参数的简单半经验公式。离子的两个外层电子,以及单个内壳电离过程,然后进行电离,再加上电子,这在我们之前的论文中已经提到过(Shevelko等,2005)。发现在那里获得的公式很好地描述了可用的实验性双电离截面,准确度为20-30%。但是,对于多电子,在低能区发现非常重的离子,该式与实验的显着偏离。这些偏差最有可能是由高阶过程引起的,包括内壳激发和随后的双重自电离(EDA)。列出的参数可用于在实验室和天体等离子体的建模中轻松分析重质正离子的双电离截面。

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