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Two-electron dynamics in nonlinear double excitation of helium by intense ultrashort extreme-ultraviolet pulses

机译:强烈的超短极紫外脉冲对氦气的非线性双重激发中的双电子动力学

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摘要

We present a theoretical study for multiphoton double excitation of He atoms exposed to an intense ultrashort extreme-ultraviolet (EUV) pulse, where the photon energy coincides with the transition energy from the ground state to a Rydberg state, by solving the time-dependent Schr?dinger equation in the hyperspherical coordinates. Photoelectron spectra under the conditions comparable with a recent experiment [Hishikawa, Phys. Rev. Lett.PRLTAO0031- 900710.1103/PhysRevLett.107.243003 107, 243003 (2011)] are calculated and analyzed. We identify the mechanism of the enhanced three-photon absorption probability which is more than one order of magnitude larger than that for the two-photon process in accordance with the experiment. The enhancement is attributed to a propensity rule for double excitation in a two-step mechanism, in which a one-photon absorption by one electron to a Rydberg state is followed by a two-photon absorption by the other electron to an excited orbital, while the first electron remains at nearly the same principle quantum number. Based on the time-dependent perturbation theory, the three-photon absorption probability exhibits peculiar cubic dependence on the pulse duration due to the propensity rule, in contrast to the linear dependence of the two-photon absorption probability. Thus a crossover between the two- and three-photon absorption probabilities takes place for sufficiently intense and long pulses. We also study the time evolution of a doubly excited two-electron wave packet created by an intense ultrashort EUV pulse efficiently using the same enhancement scheme, opening up the possibility of visualizing the correlated motion of two electrons in the time domain.
机译:我们提出了一个理论研究,用于对He原子在强超短超紫外(EUV)脉冲下的多光子双激发进行研究,其中光子能量与从基态到Rydberg态的跃迁能重合,通过解决与时间有关的Schr超球坐标系中的Fdinger方程。在与最近的实验相当的条件下的光电子能谱[Hishikawa,Phys。 Rev.Lett.PRLTAO0031- 900710.1103 / PhysRevLett.107.243003 107,243003(2011)]的计算和分析。根据实验,我们确定了增强的三光子吸收概率的机制,其比两光子过程的吸收能力大一个数量级。增强归因于在两步机制中双激发的倾向性规则,其中一个电子将一个光子吸收到里德堡态,然后另一个电子将两个光子吸收到一个受激轨道,而第一电子保持几乎相同的主量子数。基于时变摄动理论,与倾向性线性关系相比,由于倾向规则,三光子吸收概率对脉冲持续时间表现出独特的三次依赖性。因此,对于足够强和长的脉冲,在两个和三个光子吸收概率之间发生交叉。我们还研究了使用相同的增强方案有效地由强超短EUV脉冲产生的双激发双电子波包的时间演化,从而打开了可视化时域中两个电子的相关运动的可能性。

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