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Sequential and nonsequential double ionization of helium by intense XUV laser pulses: Revealing ac Stark shifts from joint energy spectra

机译:激光XUV激光脉冲氦的顺序和非顺序双电离:揭示关节能谱的AC STARK偏移

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摘要

Double ionization of a model helium system by intense extreme ultraviolet laser pulses is investigated by solving the time-dependent Schrodinger equation and extracting the photoelectron spectra. Considering a frequency regime where the nonsequential two-photon double ionization is expected to dominate the double ionization process according to the perturbation theory, we identify the sequential and nonsequential mechanisms from the joint energy spectra of two electrons in the strong-field regime. In the nonperturbative regime, we find that sequential multiphoton double ionization shows remarkable peaks in the joint energy spectra and these peaks spread their widths with increasing laser field strength, which is caused by the ac Stark effect. Thus in the strong-field regime, the ac Stark shifts of different ionic states can be observed from the sequential multiphoton features in the joint energy spectra and the signs of the ac Stark shifts can be controlled by the laser frequency. We also find that the nonsequential mechanism dominates double ionization only at low field strengths while the sequential multiphoton mechanism contributes substantially at high field strengths, in accordance with estimates from rate equations.
机译:通过求解时间依赖的Schrodinger方程并提取光电子谱来研究通过强烈的极端紫外激光脉冲进行模型氦系统的双电离。考虑到预期非顺强性双光子双电离的频率调节,预期根据扰动理论占据双电离过程,我们在强大的场地中识别来自两个电子的关节能谱的顺序和非顺序机制。在非触发状态下,我们发现序贯多光子双电离显示在关节能谱中显示出显着的峰值,并且这些峰值随着激光场强的增加而扩散它们的宽度,这是由AC颗粒效应引起的。因此,在强场方案中,可以从关节能谱中的顺序多光子特征观察不同离子状态的AC STARK偏移,并且可以通过激光频率控制交流STARK偏移的符号。我们还发现,根据速率方程的估计,在低场强度下,仅在低场强度下占据了双电离的双电离机制。

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