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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:来自时间相关的薛定inger方程的解的EUV氦的两个光子电离截面,并与使用自由电子激光器的测量结果进行比较

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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:最近的两篇实验论文报道了使用自由电子激光(FEL)脉冲对EUV波长的氦气的绝对双光子电离截面sigma(2)的首次测量[Sato等,J。Phys。 B 44,161001(2011); Fushitani等,Phys。 Rev.A 88,063422(2013)]。波长对应于与1s2p和1s3p(1Po)Rydberg态不共振以及共振时的跃迁。对它们的结果的检查发现了相当大的差异,而将它们与早先从与时间无关的计算中获得的理论结果(一个扰动和两个非扰动的计算)进行比较,则无法得出关于sigma(2)真实值的可靠结论。我们通过实施时变方法来研究此原型问题,该方法利用了时变Schr odinger方程的非摄动解。该解决方案是根据状态特定的扩展方法获得的,在升级版本中耦合矩阵元素是使用多极哈密顿量的全电算子计算的,与2011 FEL实验一样,对于300 fs的脉冲获得sigma(2),其计算是通过将随时间变化的电离存活概率拟合为e(- Gamma t),其中Gamma是电离速率,波长和强度是FEL实验的波长和强度,以及其他波长和强度,例如波长52.22和51.56 nm,其中1s4p P-1(o)和1s5p P -1(o)水平与初始S-1状态共振,除了对这些波长的预测之外,本文还对这些EUV sigma(2),实验和理论上的所有结果进行了特征比较。 tic。通常,非扰动方法预测的趋势通过FEL测量得到证实。但是,绝对数之间存在差异。此外,对三种非扰动方法(目前的时间依赖性方法和1999年和2005年发布的两种较早的时间依赖性方法)的结果进行比较表明,总体上是一致的,尽管各个案例的数量差异是显而易见的。

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