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Vacuum electron acceleration by an intense laser

Abstract

Using 3D test particle simulations, the characteristics and essential conditions under which an electron, in a vacuum laser beam, can undergo a capture and acceleration scenario (CAS). When a_o > 100 the electron can be captured and violently accelerated to energies > 1 GeV, with an acceleration gradient > 10 GeV/cm, where a_o = eE_o/m_c wc is the normalized laser field amplitude. The physical mechanism behind the CAS is that diffraction of the focused laser beam leads to a slowing down of the effective wave phase velocity along the captured electron trajectory, such that the electron can be trapped in the acceleration phase of the wave for a longer time and thus gain significant energy from the field.

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