短激光脉冲使原子电离:共振和干涉效应

A. Kondorskiy, L. Presnyakov
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引用次数: 2

摘要

研究了强电磁场作用下原子相互作用的动力学。在求解时变薛定谔方程的紧密耦合方法的基础上,建立了短激光脉冲原子电离和激发理论。研究原子与强电磁场的相互作用需要使用系统的所有连续状态,而不需要对连续体进行离散化。本文系统地研究了线偏振和圆偏振飞秒激光脉冲的激光频率、光强和持续时间的不同取值。发现中间离散态与连续态(无束缚跃迁)的相互作用对喷射电子能谱的结构非常重要。结果表明,在弹射电子的中等能量下,这些无束缚跃迁比重散射过程(自由-自由跃迁)的贡献更大。在h原子和类h离子的情况下,离散态和连续态原子居群中的共振和干涉结构表现为激光脉冲参数的函数。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Ionization of atoms by short laser pulses: resonance and interference effects
Dynamics of the interactions of atoms with intense electromagnetic fields is considered. The theory of ionization and excitation of atoms by the short laser pulses is developed on the basis of the close-coupling approach for solving the time-dependent Schrodinger equation. Studies of the interactions of atoms with intense electromagnetic fields require the use all the continuous states of the system, without discretization of the continuum. The systematic investigations have been done in the case of femtosecond laser pulses with linear and circular polarization, for the different vlaues of the laser frequency, intensity and duration times. Interactions of the intermediate discrete states with the continuum (bound-free transitions) are found to be very important for structures of the energy spectra of the ejected electrons. It is shown that these bound-free transitions give the larger contributions than the rescattering process (free-free transitions) at the medium energies of the ejected electrons. The resonance and interference structures in populations of the discrete and continuum atomic states are displayed as functions of the laser pulse parameters in the case of the H-atoms and H-like ions.
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