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Classical and quantum-mechanical scaling of ionization from excited hydrogen atoms in single-cycle THz pulses

机译:单循环THz脉冲中的激发氢原子离子化的经典和量子机械缩放

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摘要

Excited atoms, or nanotip surfaces, exposed to strong single-cycle terahertz radiation emit electrons with energies strongly dependent on the characteristics of the initial state. Here we consider scaling properties of the ionization probability and electron momenta of H(nd) atoms exposed to a single-cycle pulse of duration 0.5-5 ps, with n = 9,12,15. Results from three-dimensional quantum and classical calculations are in good agreement for long pulse lengths, independent of pulse strength. However, differences appear when the two approaches are compared at the most detailed level of density distributions. For the longest pulse lengths a mixed power law, n-scaling relation, αn~(-4) + (1 - α)n~(-3) is shown to hold. Our quantum calculations show that the scaling relation puts its imprint on the momentum distribution of the ionized electrons as well: By multiplying the emitted electron momenta of varying initial n level with the appropriate scaling factor the spectra fall onto a common momentum range. Furthermore, the characteristic momenta of emitted electrons from a fixed n level are proportional to the pulse strength of the driving field.
机译:激发原子或纳米坡面,暴露于强的单循环太赫兹辐射发射电子,其能量强烈地取决于初始状态的特性。在这里,我们认为H(nd)原子的电离概率和电子动势的缩放性质暴露于持续时间0.5-5 ps的单循环脉冲,n = 9,12,15。三维量子和经典计算的结果与长脉冲长度相一致,与脉冲强度无关。然而,当在最详细的密度分布水平上比较两种方法时,差异出现。对于最长的脉冲长度,混合动力定律,N形缩放关系,αn〜(-4)+(1 - α)n〜(-3)被显示为保持。我们的量子计算表明,缩放关系对电离电子的动量分布的缩放表示:通过将所发射的电子动量乘以不同初始n水平的发射电子动量,该光谱落入常见的动量范围。此外,来自固定N电平的发射电子的特征动量与驱动场的脉冲强度成比例。

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