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Floquet analysis of real-time wave functions without solving the Floquet equation

机译:不求解Floquet方程的实时波动函数的Floquet分析

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We propose a method to obtain Floquet states—also known as light-induced states—and their quasienergies from real-time wave functions without solving the Floquet equation. This is useful for the analysis of various phenomena in time-dependent quantum dynamics if the Hamiltonian is not strictly periodic, as in short laser pulses, for instance. There, the population of the Floquet states depends on the pulse form and is automatically contained in the real-time wave function but not in the standard Floquet approach. Several examples in the area of intense laser-atom interaction are exemplarily discussed: (i) the observation of even harmonics for an inversion-symmetric potential with a single bound state; (ii) the dependence of the population of Floquet states on (gauge) transformations and the emergence of an invariant, observable photoelectron spectrum; (iii) the driving of resonant transitions between dressed states, (i.e., the dressing of dressed states), and (iv) spectral enhancements at channel closings due to the ponderomotive shift of above-threshold ionization peaks.
机译:我们提出了一种无需求解Floquet方程即可从实时波函数获得Floquet状态(也称为光诱导状态)及其准能量的方法。如果哈密顿量不是严格周期性的,例如对于短激光脉冲,这对于分析随时间变化的量子动力学中的各种现象很有用。在那里,浮球状态的填充取决于脉冲形式,并自动包含在实时波函数中,但不包含在标准浮球方法中。示例性地讨论了在强烈的激光-原子相互作用领域中的几个例子:(i)对于具有单束缚态的反对称电位的偶次谐波的观察; (ii)Floquet态种群对(规范)转换的依赖性以及不变的,可观察的光电子谱的出现; (iii)在修整状态之间(即修整状态的修整)之间共振转变的驱动,以及(iv)由于高于阈值的电离峰的重动力移动,通道关闭处的频谱增强。

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