Abstract

We demonstrate a sharp density transition for electron injection in laser wakefield acceleration through numerical study. This density transition is generated by a detached shock wave induced by a cylinder inserted into a supersonic helium gas flow. In a Mach 1.5 flow, the scale length of the density transition ${L}_{\mathrm{grad}}$ can approximately equal to plasma wavelength ${\ensuremath{\lambda}}_{p}$ at the shock front, and can be further reduced with an increase of the flow Mach number. A density down ramp with ${L}_{\mathrm{grad}}\ensuremath{\ge}{\ensuremath{\lambda}}_{p}$ can reduce the phase velocity of the wakefield and lower the energy threshold for the electrons to be trapped. Moreover, the quality of the accelerated beam may be greatly improved by precisely controlling of ${L}_{\mathrm{grad}}$ to be one ${\ensuremath{\lambda}}_{p}$. For an even sharper density down ramp with ${L}_{\mathrm{grad}}\ensuremath{\ll}{\ensuremath{\lambda}}_{p}$, the oscillating electrons in the plasma wave will up shift their phase when crossing the ramp, therefore a fraction of the electrons are injected into the accelerating field. For this injection mechanism, there is no threshold requirement for the pump laser intensity to reach wave breaking, which is a big advantage as compared with other injection mechanisms.

Highlights

  • We demonstrate a sharp density transition for electron injection in laser wakefield acceleration through numerical study

  • In laser wakefield accelerators (LWFA), a wakefield driven by a high intensity laser can sustain an extremely high electric field up to 100 GV=m, 3 orders of magnitude larger than those obtained in conventional radio-frequency linear accelerators [1]

  • Different from the laser heating method, here we propose a shock wave scheme to achieve a sharp density ramp required by the injection methods of Suk [10] and Bulanov [13]

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Summary

Introduction

In laser wakefield accelerators (LWFA), a wakefield driven by a high intensity laser can sustain an extremely high electric field up to 100 GV=m, 3 orders of magnitude larger than those obtained in conventional radio-frequency linear accelerators [1]. If an electron bunch is injected into a wakefield such that it is accelerated while maintaining a small energy spread, it is necessary for the bunch to be a fraction of p and located at the appropriate phase of the wakefield with sufficient initial energy. This requires the femtosecond electron bunch to be injected with femtosecond timing accuracy. Several ways can fulfill these requirements and realize the injection of electrons: (1) self-injection in the so-called bubble region; (2) optical injection by colliding laser beams; (3) injection in a density down ramp.

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