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Supercontinuum in ionization by relativistically intense and short laser pulses: Ionization without interference and its time analysis

机译:通过相对强烈和短激光脉冲进行电离的超连续谱:无干扰的电离及其时间分析

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摘要

Ionization by relativistically intense laser pulses of finite duration is considered in the framework of strongfield quantum electrodynamics. We show that the resulting ionization spectra change their behavior from the interference-dominated oscillatory pattern to the interference-free smooth supercontinuum, the latter being the main focus of this paper. More specifically, when studying the energy distributions of photoelectrons ionized by circularly polarized and short pulses, we observe the appearance of broad structures lacking the interference patterns. These supercontinua extend over hundreds of driving photon energies, thus corresponding to high-order nonlinear processes. Their positions on the electron energy scale can be controlled by changing the pulse duration. The corresponding polar-angle distributions show asymmetries which are attributed to the radiation pressure experienced by photoelectrons. Moreover, our time analysis shows that the electrons comprising the supercontinuum can form pulses of short duration. While we present the fully numerical results, their interpretation is based on the saddle-point approximation for the ionization probability amplitude.
机译:在强场量子电动力学的框架内考虑了有限时程的相对论性强激光脉冲的电离作用。我们表明,所得的电离光谱将其行为从以干扰为主的振荡模式改变为无干扰的光滑超连续谱,后者是本文的主要重点。更具体地,当研究由圆偏振和短脉冲电离的光电子的能量分布时,我们观察到缺乏干涉图案的宽结构的出现。这些超连续谱扩展了数百个驱动光子能量,因此对应于高阶非线性过程。它们在电子能级上的位置可以通过改变脉冲持续时间来控制。相应的极角分布显示出不对称性,其归因于光电子所经历的辐射压力。此外,我们的时间分析表明,构成超连续谱的电子可以形成短持续时间的脉冲。虽然我们提供了完整的数值结果,但它们的解释是基于电离概率幅度的鞍点近似。

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