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Momentum Distribution of Near-Zero-Energy Photoelectrons in the Strong-Field Tunneling Ionization in the Long Wavelength Limit

机译:长波长范围内强场隧穿电离中近零能量光电子的动量分布

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We investigate the ionization dynamics of Argon atoms irradiated by an ultrashort intense laser of a wavelength up to 3100?nm, addressing the momentum distribution of the photoelectrons with near-zero-energy. We find a surprising accumulation in the momentum distribution corresponding to meV energy and a “V”-like structure at the slightly larger transverse momenta. Semiclassical simulations indicate the crucial role of the Coulomb attraction between the escaping electron and the remaining ion at an extremely large distance. Tracing back classical trajectories, we find the tunneling electrons born in a certain window of the field phase and transverse velocity are responsible for the striking accumulation. Our theoretical results are consistent with recent meV-resolved high-precision measurements.
机译:我们研究了波长达3100?nm的超短强激光照射的氩原子的电离动力学,解决了光电子的动量分布接近零的问题。我们发现,在稍大的横向动量处,对应于meV能量和“ V”形结构的动量分布中出现了令人惊讶的积累。半经典模拟表明,在极远距离处,逃逸的电子与剩余离子之间的库仑吸引作用至关重要。追溯经典轨迹,我们发现在场相位和横向速度的某个窗口中出生的隧穿电子是引起撞击积累的原因。我们的理论结果与最近通过meV解析的高精度测量结果一致。

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