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首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Precision calculation of above-threshold multiphoton ionization in intense short-wavelength laser fields: The momentum-space approach and time-dependent generalized pseudospectral method
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Precision calculation of above-threshold multiphoton ionization in intense short-wavelength laser fields: The momentum-space approach and time-dependent generalized pseudospectral method

机译:短波长强激光场中阈值以上多光子电离的精确计算:动量空间法和时变广义伪谱法

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摘要

We present an approach in momentum (P) space for the accurate study of multiphoton and above-threshold ionization (ATI) dynamics of atomic systems driven by intense laser fields. In this approach, the electron wave function is calculated by solving the P-space time-dependent Schrodinger equation (TDSE) in a finite P-space volume under a simple zero asymptotic boundary condition. The P-space TDSE is propagated accurately and efficiently by means of the time-dependent generalized pseudospectral method with optimal momentum grid discretization and a split-operator time propagator in the energy representation. The differential ionization probabilities are calculated directly from the continuum-state wave function obtained by projecting the total electron wave function onto the continuum-state subspace using the projection operator constructed by the continuum eigenfunctions of the unperturbed Hamiltonian. As a case study, we apply this approach to the nonperturbative study of the multiphoton and ATI dynamics of a hydrogen atom exposed to intense short-wavelength laser fields. High-resolution photoelectron energy-angular distribution and ATI spectra have been obtained. We find that with the increase of the laser intensity, the photoelectron energy-angular distribution changes from circular to dumbbell shaped and is squeezed along the laser field direction. We also explore the change of the maximum photoelectron energy with laser intensity and strong-field atomic stabilization phenomenon in detail.
机译:我们提出一种在动量(P)空间中用于精确研究由强激光场驱动的原子系统的多光子和阈值以上电离(ATI)动力学的方法。在这种方法中,通过在简单的零渐近边界条件下,在有限的P空间体积中求解P空间随时间变化的薛定inger方程(TDSE),可以计算出电子波函数。通过具有最佳动量网格离散化的时变广义伪谱方法和能量表示中的分裂算子时间传播子,可以精确有效地传播P空间TDSE。通过使用由不受干扰的哈密顿量的连续本征函数构造的投影算子,将总电子波函数投影到连续态子空间上而获得的连续态波函数,直接计算差分电离概率。作为案例研究,我们将这种方法应用于暴露于强短波激光场的氢原子的多光子和ATI动力学的非扰动研究。获得了高分辨率的光电子能角分布和ATI光谱。我们发现随着激光强度的增加,光电子的能量角分布从圆形变为哑铃形,并沿激光场方向受到挤压。我们还将详细研究最大光电子能量随激光强度和强场原子稳定现象的变化。

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