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首页> 外文期刊>Physical Review, A >EUV two-photon-ionization cross sections of helium from the solution of the time-dependent Schrodinger equation, and comparison with measurements using free-electron lasers
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EUV two-photon-ionization cross sections of helium from the solution of the time-dependent Schrodinger equation, and comparison with measurements using free-electron lasers

机译:从时间依赖性Schrodinger方程的溶液中氦的EUV双光子电离横截面,并使用自由电子激光测量比较

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摘要

Two recent experimental papers reported the first measurements of absolute two-photon-ionization cross sections sigma(2) of helium, for EUV wavelengths, using free-electron laser (FEL) pulses [Sato et al., J. Phys. B 44, 161001 (2011); Fushitani et al., Phys. Rev. A 88, 063422 (2013)]. The wavelengths correspond to transitions that are off resonance as well as on resonance with the 1s2p and 1s3p(1Po) Rydberg states. Inspection of their results reveals considerable discrepancies, while their comparison with theoretical results obtained earlier from time-independent calculations, one perturbative and two nonperturbative ones, cannot lead to secure conclusions as to the true values of sigma(2). We examined this prototypical problem by implementing a time-dependent approach, which utilizes the nonperturbative solution of the time-dependent Schr " odinger equation. This solution was obtained in terms of the state-specific expansion approach, in an upgraded version where the coupling matrix elements are computed using the full electric operator of the multipolar Hamiltonian. The sigma(2) were obtained for pulses of 300 fs, as in the 2011 FEL experiment. Their computation was achieved by fitting the time-dependent ionization survival probability to e(-Gamma t), where Gamma is the rate of ionization. The wavelengths and intensities are those of the FEL experiments, as well as others, such as the wavelengths 52.22 and 51.56 nm, for which the 1s4p P-1(o) and 1s5p P-1(o) levels are on resonance with the initial S-1 state. Apart from the predictions for these wavelengths, the paper contains characteristic comparisons among all the results on these EUV sigma(2), experimental and theoretical. In general, the trends predicted by nonperturbative methods are confirmed by the FEL measurements. However, discrepancies exist among the absolute numbers. Furthermore, comparison among the results of the three nonperturbative approaches (present time-dependent and two earlier time-independent ones published in 1999 and 2005) indicates an overall consistency, although quantitative differences for individual cases are apparent.
机译:最近的两个实验纸报道,使用自由电子激光器(FEL)脉冲[Sato等人,J. phys,首先报道了Euv波长的绝对双光子电离横截面Sigma(2)的第一次测量。 B 44,161001(2011); Fushitani等人。,phy。 Rev. A 88,063422(2013)]。波长对应于截止谐振的转换以及与1S2P和1S3P(1PO)Rydberg状态的谐振。检查结果的检查揭示了相当大的差异,而他们与早期从多余的计算中获得的理论结果的比较,一个扰动和两个非植牢性的结果,不能导致Sigma(2)的真实价值的确保结论。我们通过实施时间依赖性方法来检查该原型问题,该方法利用时间依赖的SCHR“odinger方程的非触发解。在耦合矩阵的升级版本中,在状态特定的扩展方法方面获得了该解决方案使用多极汉密尔顿人的全电动操作员计算元素。如2011年FIR实验中,获得了300 FS脉冲的Sigma(2)。通过将时间依赖性电离存活概率拟合到E( - γT),其中γ是电离速率。波长和强度是FEL实验的,以及其他波长52.22和51.56nm,其中1S4P P-1(O)和1S5P P. -1(o)水平与初始S-1状态相谐振。除了这些波长的预测外,本文还包含这些EUV Sigma(2),实验和致命的所有结果的特征比较tical。通常,通过FEL测量确认了非触发方法预测的趋势。但是,绝对数字之间存在差异。此外,三种非培育方法的结果(现在依赖于1999年和2005年出版的两年前的时间和两个较早的时间依赖性的)的比较表明了整体一致性,尽管个体病例的定量差异是明显的。

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