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Modeling the interaction between a few-cycle relativistic laser pulse and a plasma mirror : from electron acceleration to harmonic generation

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Academic year: 2021

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Figure

Table 1.1: Conversion table between practical quantities for theory and experiments.
Figure 1.1: Schematic of a plasma mirror. The laser pulse is obliquely-incident, p-polarized, ultraintense (a 0 ∼ 1) and ultrashort (τ ∼ 25 fs)
Figure 1.2: Appropriate description depending on the plasma parameters. BBGKY stands for Bogoliubov-Born-Green-Kirkwood-Yvon.
Figure 1.3: (a) The external electric field is weak, the atom binding potential is not distorted and the prevailing mechanism is multiphoton ionization
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