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Floquet Scattering and Classical-Quantum correspondence in strong time periodic fields

机译:强时间周期场中的浮球散射和古典-量子对应

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摘要

We study the scattering of an electron from an inverted Gaussian atomic potential in the presence of strong time periodic electric fields. Using Floquet theory, we construct the Floquet Scattering matrix in the Kramers-Henneberger frame. We compute the transmission coefficients as a function of electron incident energy and find that they display asymmetric Fano resonances due to the electron interaction with the driving field. We find that the Fano resonances are associated with zero-pole pairs of the Floquet Scattering matrix in the complex energy plane. Another way we "probe" the complex spectrum of the system is by computing the Wigner delay times. Finally we find that the eigenphases of the Floquet Scattering matrix undergo a number of "avoided crossings" as a function of electron incident energy that increases with increasing strength of the driving field. These "avoided crossings" appear to be quantum manifestations of the destruction of the constants of motion and the onset of chaos in classical phase space.
机译:我们研究了在强时间周期电场存在下电子从反向高斯原子势的散射。使用Floquet理论,我们在Kramers-Henneberger框架中构造了Floquet散射矩阵。我们计算了作为电子入射能量的函数的传输系数,发现由于电子与驱动场的相互作用,它们显示出不对称的Fano共振。我们发现,Fano共振与复能平面中的Floquet散射矩阵的零极点对相关。我们“探测”系统复杂频谱的另一种方法是计算威格纳延迟时间。最终,我们发现,浮子散射矩阵的本征相随着电子入射能量的变化而经历了许多“避免的穿越”,电子入射能量随着驱动场强度的增加而增加。这些“避免的交叉”似乎是经典相空间中运动常数的破坏和混沌的开始的量子表现。

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