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Disentangling intracycle interferences in the photoelectron spectrum of argon using orthogonally polarized, two-colour laser pulses

机译:使用正交偏振,双色激光脉冲解开氩光电子光谱中的血管光谱干扰

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In recent years, the widespread availability of multi-dimensional photoelectron spectroscopy has created the opportunity to systematically study the complex interference patterns inherent to multiphoton ionization of atoms and molecules. The dominant interference mechanism in multiphoton ionization leads to discrete peaks in the photoelectron spectrum (PES) that are spaced by the photon energy of the driving laser field. This mechanism is called above-threshold ionization (ATI) and has its origin in the coherence of ionization events repeating at every oscillation of the optical field [1]. However, many more interference mechanisms contribute to the observed photoelectron spectrum. Specifically, photoelectrons emitted within one cycle of the optical field can also interfere on the detector. These interferences from photoelectrons originating in adjacent quarter-cycles of the optical field are also known as the temporal double slit (e.g., [1]). In addition, scattering of the photoelectron on the parent ion potential will give rise to holographic interferences [2], and laser induced electron diffraction [3].
机译:近年来,多维光电子光谱的广泛可用性已经创造了系统地研究了原子和分子的多选电离所固有的复杂干扰模式的机会。多光电电离中的主导干扰机制导致光电子光谱(PE)中的离散峰,其由驱动激光场的光子能量间隔开。该机制被称为高于阈值电离(ATI),并且其起源在光学场的每个振荡时重复的电离事件的相干事件中的起源[1]。然而,许多更多的干扰机制有助于观察到的光电子光谱。具体地,在光场的一个循环中发射的光电子也可以干扰检测器。来自光学场的相邻四分之一循环的光电子的这些干扰也称为时间双狭缝(例如,[1])。另外,光电子对母体离子电位的散射将导致全息干扰[2],激光诱导电子衍射[3]。

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