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Resonant two- or three-photon ionization of noble-gas atoms captured by time-resolved photoelectron momentum spectroscopy

机译:通过时间分辨的光电子电量光谱捕获的贵瓦气原子的共振两级或三光子电离

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We present an all-electron, ab initio calculation of time-resolved photoelectron momentum distributions (PMDs) induced by resonant two-color, two- or three-photon ionization of helium and neon atoms, as recently measured by Villeneuve et al. [Science 356, 1150 (2017)] using a femtosecond infrared (IR) laser pulse and an attosecond pulse train (APT) produced with high harmonic generation as an extreme ultraviolet (XUV) photon source. In contrast to a monochromatic XUV pulse commonly used at the free-electron laser facilities, an APT is broadband and ultrashort (<1 fs), so that it could induce nonresonant one-photon transitions above ionization threshold as well as a resonantly excited state. They may interfere with each other upon subsequent absorption or emission of an IR photon, so that the resultant PMD loses clear orbital symmetry. Our time-dependent density functional calculation demonstrates that the selection of a particular excited state in the time-resolved PMD is nevertheless possible if energy and timing of an APT are adjusted properly.
机译:我们介绍了通过Villeneuve等人测量的氦气和氖原子的谐振双色,两种或三光子电离诱导的时间分辨的光电子动量分布(PMD)的全电子AB初始化。 [Science 356,1150(2017)]使用飞秒红外(IR)激光脉冲和具有高谐波产生的AttoSecond脉冲列车(APT)作为极端紫外线(XUV)光子源。与常用于自由电子激光器设施的单色XUV脉冲相反,APT是宽带和超短(<1FS),因此它可以诱导高于电离阈值的非族化单光子转变以及谐振激发的状态。它们可以在随后的吸收或发射红外光子的吸收或发射时彼此干扰,因此所得PMD失去透明轨道对称性。我们的时间依赖性密度函数计算表明,如果适当调整APT的能量和时序,则可能在分辨的PMD中选择特定激发状态。

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