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Numerical simulation of time delays in light induced ionization

机译:光诱导电离时间延迟的数值模拟

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摘要

We apply a fundamental definition of time delay, as the difference betweenthe time a particle spends within a finite region of a potential and the time afree particle spends in the same region, to determine results forphotoionization of an electron by an extreme ultraviolet (XUV) laser fieldusing numerical simulations on a grid. Our numerical results are in goodagreement with those of the Wigner-Smith time delay, obtained as the derivativeof the phase shift of the scattering wave packet with respect to its energy,for the short-range Yukawa potential. In case of the Coulomb potential weobtain time delays for any finite region, while - as expected - the results donot converge as the size of the region increases towards infinity. The impactof an ultrashort near-infrared probe pulse on the time delay is analyzed forboth the Yukawa as well as the Coulomb potential and is found to be small forintensities below $10^{13}$ W/cm$^2$.
机译:我们使用时间延迟的基本定义,即粒子在电势的有限区域内停留的时间与游离粒子在同一区域内停留的时间之间的差,以确定通过极紫外(XUV)激光进行电子光电离的结果使用网格上的数值模拟进行现场。我们的数值结果与Wigner-Smith时延的数值非常吻合,后者是散射波包相对于其能量的短距离汤川势的相移导数。在库仑电势的情况下,对于任何有限区域,我们都会获得时间延迟,而正如预期的那样,结果不会随着区域的大小向无穷大增加而收敛。分析了Yukawa以及库仑电势的超短近红外探测脉冲对时间延迟的影响,发现对于低于$ 10 ^ {13} $ W / cm $ ^ 2 $的强度来说,这种影响很小。

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