Du Hongchuan, Wu Hongmei, Wang Huiqiao, Yue Shengjun, Hu Bitao
Opt Lett. 2016 Feb 15;41(4):697-700. doi: 10.1364/OL.41.000697.
Photoelectron angular momentum distribution of He driven by a few-cycle laser is investigated numerically. We simultaneously observe two dominant interference patterns with one shot of lasers by solving the 3D time-dependent Schrodinger equation. Analysis of a semiclassical model identifies these two interference patterns as two types of photoelectron holography. The interference pattern with P>0 is a type of forward rescattering holography, which comes from the interference between direct (reference) and rescattered (signal) forward electrons ionized in the same quarter-cycle. The interference pattern with P<0 is a type of backward rescattering holography, which comes from the interference between a direct electron ionized in the third quarter-cycle and rescattered backward electron ionized in the first quarter-cycle. Moreover, we propose a method to distinguish this backward rescattering holography and intracycle interference patterns of direct electrons.
对由几周期激光驱动的氦原子的光电子角动量分布进行了数值研究。通过求解三维含时薛定谔方程,我们用单次激光照射同时观测到了两种主要的干涉图样。半经典模型分析将这两种干涉图样识别为两种类型的光电子全息术。P>0的干涉图样是一种前向再散射全息术,它来自于在同一四分之一周期内电离的直接(参考)和再散射(信号)前向电子之间的干涉。P<0的干涉图样是一种后向再散射全息术,它来自于在第三四分之一周期内电离的直接电子与在第一四分之一周期内再散射的后向电子之间的干涉。此外,我们提出了一种区分这种后向再散射全息术和直接电子的周期内干涉图样的方法。