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arXiv 0712.0695physics.atom-phphysics.comp-ph
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强超短脉冲laser电离氢原子

Ionization of the hydrogen atom by intense ultrashort laser pulses

S. Borbély, K. Tőkési, L. Nagy

摘要:

从理论上研究了强激光场中氢原子的电离。应用量子力学和经典方法进行计算。从量子力学的角度出发,首先将系统的含时薛定谔方程(TDSE)变换到赝动量空间中,并在赝动量空间中迭代求解。在求解TDSE时忽略库仑势的影响,得到了Volkov近似下的结果,在一阶解中考虑了库仑势作为微扰。经典的计算框架内进行的经典轨迹蒙特卡罗(CTMC)方法。计算了不同激光脉冲下的双微分电离几率,理论结果与实验结果吻合较好。在低电子能量下,经典方法和量子力学方法之间的电子角分布可以观察到重大差异。当电子能量较高时,这种差异消失,表明低能电子的产生是量子型的,受库仑势的影响很大,而高能电子的产生是经典型的,受库仑相互作用的影响较小.我们的结果也比较了库仑-Volkov(CV)模型的计算。

英文摘要:

The ionization of atomic hydrogen in intense laser fields is studied theoretically. The calculations were performed applying both quantummechanical and classical approaches. Treating the problem quantummechanically, the time dependent Schrödinger equation (TDSE) of our system was first transformed into a pseudo-momentum space and solved in this space iteratively. While neglecting the Coulomb potential during the solution of the TDSE we got the results in the Volkov approximation, in the first order solution we taken into account the Coulomb potential as perturbation. The classical calculations were performed within the framework of the classical trajectory Monte-Carlo (CTMC) method. The double differential ionization probabilities are calculated for different laser pulses and a reasonable agreement was found between the theories. Major differences can be observed in the angular distribution of electrons at low electron energies between classical and the quantummechanical approaches. At high electron energies the differences disappear, which indicates that the generation of low energy electrons is of quantum type, and it is strongly influenced by the Coulomb potential, while the production of high energy electrons is of classical type and it is less influenced by the Coulomb interaction. Our results are also compared with the Coulomb-Volkov (CV) model calculations.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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