K. Schrick, K. H. Spicer, N. W. Antonio, Sh. U. Alladustov, A. S. Kadyrov
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引用次数: 0
摘要
在2 keV/u到3 MeV/u的弹丸能量范围内,使用双中心四体波包收敛紧密耦合方法计算了C \(^{6+}-\) He碰撞中总电子捕获和状态选择电子捕获和电离的集成截面。双电子靶结构解释了电子-电子相关效应,以及重排C \(^{5+}-\) He \(^{+}\)通道中的电子交换,这在低能和中能时变得重要。还用于比较的是另一种方法,将He目标降低到有效的单电子系统。对于电子捕获,两种方法在高冲击能量下与实验结果一致。对于低冲击能量,双电子方法表现良好,然而,有效的单电子模型高估了现有的实验数据。两种方法对能量大于100 keV/u的弹丸电离截面的计算结果与实验结果基本吻合。有效的单电子方法被扩展到10 keV/u,但它高估了低能实验。结论是,为了在整个入射碰撞能量范围内正确地模拟电子捕获,双电子目标描述是必要的。
Electron capture and ionisation in intermediate-energy C\(^{6+}-\)He collisions: Integrated cross sections
Integrated cross sections for total and state-selective electron capture, and ionisation in C\(^{6+}-\)He collisions are calculated using the two-centre four-body wave-packet convergent close-coupling method for projectile energies ranging from 2 keV/u to 3 MeV/u. The two-electron target structure accounts for electron-electron correlation effects, as well as electron exchange in the rearrangement C\(^{5+}-\)He\(^{+}\) channels, which become important at low and intermediate energies. Also used for comparison is an alternative approach that reduces the He target to an effective one-electron system. For electron capture, both methods display good agreement with experiments at high impact energies. For low impact energies the two-electron method performs well, however, the effective single-electron model overestimates available experimental data. Generally good agreement with experiment is found for ionisation cross sections for projectile energies greater than 100 keV/u with both methods. The effective single-electron method is extended down to 10 keV/u, however it overestimates low-energy experiments. It is concluded that the two-electron target description is necessary to correctly model electron capture in the entire range of incident collision energies considered in this work.
期刊介绍:
The European Physical Journal D (EPJ D) presents new and original research results in:
Atomic Physics;
Molecular Physics and Chemical Physics;
Atomic and Molecular Collisions;
Clusters and Nanostructures;
Plasma Physics;
Laser Cooling and Quantum Gas;
Nonlinear Dynamics;
Optical Physics;
Quantum Optics and Quantum Information;
Ultraintense and Ultrashort Laser Fields.
The range of topics covered in these areas is extensive, from Molecular Interaction and Reactivity to Spectroscopy and Thermodynamics of Clusters, from Atomic Optics to Bose-Einstein Condensation to Femtochemistry.