Abstract

A laser pulse propagating in a corrugated plasma channel is composed of spatial harmonics whose phase velocities can be subluminal. The phase velocity of a spatial harmonic can be matched to the speed of a relativistic electron resulting in direct acceleration by the guided laser field in a plasma waveguide and linear energy gain over the interaction length. Here we examine the fully self-consistent interaction of the laser pulse and electron beam using particle-in-cell (PIC) simulations. For low electron beam densities, we find that the ponderomotive force of the laser pulse pushes plasma channel electrons towards the propagation axis, which deflects the beam electrons. When the beam density is high, the space charge force of the beam drives the channel electrons off axis, providing collimation of the beam. In addition, we consider a ramped density profile for lowering the threshold energy for trapping in a subluminal spatial harmonic. By using a density ramp, the trapping energy for a normalized vector potential of ${a}_{0}=0.1$ is reduced from a relativistic factor ${\ensuremath{\gamma}}_{0}=170$ to ${\ensuremath{\gamma}}_{0}=20$.

Highlights

  • In this paper, we explore, through theory and simulations, the quasi-phase-matched direct acceleration (QPMA) of electrons in an axially modulated plasma waveguide

  • For low electron beam densities, we find that the ponderomotive force of the laser pulse pushes plasma channel electrons towards the propagation axis, which deflects the beam electrons

  • In the absence of phase-matching, a modulation in the nonlinearity or in the refractive index can be introduced along the propagation axis such that the wave vector mismatch between the two waves is provided by the effective wave vector of the structure

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Summary

INTRODUCTION

We explore, through theory and simulations, the quasi-phase-matched direct acceleration (QPMA) of electrons in an axially modulated plasma waveguide. In the scheme described here, an electron beam copropagating with a radially polarized laser pulse injected into a corrugated plasma waveguide is accelerated by a phasematched axial spatial harmonic of the resulting guided electromagnetic field, providing linear energy gain over the interaction length [2]. In order to achieve linear energy gain over an extended interaction length, three things are required: slow electromagnetic waves (providing quasiphase-matching), a channel for guiding the laser pulse (eliminating diffractive spreading of the laser pulse) [3,4], and radial polarization (providing a component of electric field along the propagation axis) [2].

CODE DETAIL AND VERIFICATION
LOW ENERGY ELECTRON ACCELERATION
Findings
SUMMARY AND CONCLUSIONS
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