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High-order harmonic generation spectrum of an excited one-dimensional Coulomb atom in an intense laser field

机译:强激光场中激发的一维库仑原子的高次谐波产生谱

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摘要

Response of the wave packet of a one-dimensional Coulomb atom to an intense laser field is calculated using the symmetrized split operator fast Fourier method. The high-order harmonic generation (HHG) of the initial state separately being the ground and excited states is presented. When the hardness parameter α in the soft Coulomb potential V(x) = -1/(x~2+α)~(1/2) is chosen to be small enough, the so-called hard Coulomb potential V(x) = -1/|x| can be obtained. It is well known that the hard one-dimensional Coulomb atom has an unstable ground state with an energy eigenvalue of ~ 0.5 and it has no states corresponding to physical states in the true atoms, and has the first and second excited states being degenerate. The parity effects on the HHG can be seen from the first and second excited states of the hard one-dimensional Coulomb atom. The HHG spectra of the excited states from both the soft and hard Coulomb atom models are shown to have more complex structures and to be much stronger than the corresponding HHG spectrum of the ground state of the soft Coulomb model with α = 2 in the same laser field. Laser-induced non-resonant one-photon emission is also observed.
机译:使用对称的分裂算子快速傅立叶方法计算一维库仑原子的波包对强激光场的响应。提出了初始状态分别为基态和激发态的高次谐波产生(HHG)。当软库仑电势V(x)= -1 /(x〜2 +α)〜(1/2)中的硬度参数α选择得足够小时,所谓的硬库仑电势V(x)= -1 / | x |可以获得。众所周知,一维硬库仑原子具有不稳定的基态,其能量本征值为〜0.5,并且不具有与真实原子中的物理状态相对应的状态,并且具有第一和第二激发态退化。从硬一维库仑原子的第一和第二激发态可以看出对HHG的奇偶效应。在相同的激光器中,来自软库仑模型和硬库仑原子模型的激发态的HHG光谱显示具有更复杂的结构,并且比具有α= 2的软库仑模型的基态的相应HHG光谱更强。领域。还观察到激光诱导的非共振单光子发射。

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