椭圆偏振激光场中不同磁量子数原子态光电子的时间能量分布

Jingyang Xu, Li Guo, Xin Qi, R. Lu, Min Zhang, Jingtao Zhang, Jing Chen
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摘要

基于强场近似(SFA)理论的 Wigner 分布样(WDL)函数被用来研究椭圆极化电场中不同磁量子数 m 的初始态发射的光电子的电离时间。采用鞍点法进行比较。对于不同的 m 状态,在靠近激光场椭圆主轴方向发射的光电子的 WDL 分布存在差异。根据鞍点分析,这种差异可归因于两个隧道瞬时电离的电子之间的干扰。我们的研究结果表明,在不考虑库仑势的情况下,不同 m 初始状态下的隧道瞬时与光电子动能之间的关系是相同的。我们的研究揭示了不同磁量子态电子的电离时间信息。
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Time-energy distribution of photoelectron from atomic states with different magnetic quantum numbers in elliptically polarized laser fields
A Wigner-distribution-like (WDL) function based on the strong-field approximation (SFA) theory is used to investigate the ionization time of the photoelectron emitted from the initial states with different magnetic quantum number m in elliptically polarized electric fields. The saddle-point method is adopted for comparison. For different m states, a discrepancy exists in the WDL distributions of the photoelectrons emitted in a direction close to the major axis of the laser field ellipse. Based on the saddle-point analysis, this discrepancy can be ascribed to the interference between electrons ionized from two tunneling instants. Our results show that the relationships between the tunneling instants and kinetic energy of the photoelectrons are the same for different m initial states when the Coulomb potential is not considered. Our work sheds some light on the ionization-time information of electrons from different magnetic quantum states.
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