Effects of Chromatic Aberration in a Dephasingless Laser Wakefield Accelerator

POSTER

Abstract

In laser wakefield accelerators, the ponderomotive force of an intense laser pulse propagating through a plasma excites a large-amplitude plasma wakefield that can trap and accelerate electrons. To overcome dephasing and prevent the electrons from outrunning the wakefield, spatiotemporal pulse shaping can be used to propagate the laser intensity at the speed of light in the plasma over long distances without the need for guiding structures. An axiparabola enables spatiotemporal control by focusing light rays at different near-field radial locations to different far-field axial locations, while maintaining a small spot size over distances greater than a Rayleigh range. To control the time at which each radius comes to its corresponding focus, a radial group delay is introduced to the shape of the pulse. Two methods to achieve this are compared: (1) a reflective, radially stepped echelon optic and (2) two specially shaped glasses. Both techniques inherently introduce k-vector spread and thereby far-field pulse broadening. The physical origins and implications of these chromatic aberrations are compared and discussed using scalar diffraction theory and ray-trace modeling.

*This material is based upon work supported by the Department of Energy National Nuclear Security Administration under Award Number DE-NA0003856 and the Department of Energy Office of Fusion Energy under Award Number DE-SC00215057.

Presenters

  • Manfred Virgil Ambat

    • Laboratory for Laser Energetics, U. of Rochester

Authors

  • Manfred Virgil Ambat

    • Laboratory for Laser Energetics, U. of Rochester
  • Robert Boni

    • Laboratory for Laser Energetics, U. of Rochester
  • Jessica Shaw

    • University of Rochester
  • Philip Franke

    • Laboratory for Laser Energetics, U. of Rochester
    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics
    • University of Rochester
  • Kyle R McMillen

    • University of Rochester
  • Matthew A VanDusen-Gross

    • Laboratory for Laser Energetics, U. of Rochester
  • Hans Rinderknecht

    • University of Rochester Laboratory for Laser Energetics
    • Laboratory for Laser Energetics, U. of Rochester
    • Laboratory for Laser Energetics - Rochester
    • Lab for Laser Energetics
    • Laboratory for Laser Energetics
    • Laboratory for Laser Energetics, University of Rochester
    • University of Rochester
  • Dillon W Ramsey

    • University of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics
  • Tanner T Simpson

    • University of Rochester
    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics
    • Laboratory for Laser Energetics, U. of Rochester
  • John P Palastro

    • Laboratory for Laser Energetics, U. of Rochester
    • Laboratory for Laser Energetics
    • University of Rochester
    • Lab for Laser Energetics
    • Laboratory for Laser Energetics, University of Rochester
  • Seung-Whan Bahk

    • Laboratory for Laser Energetics, U. of Rochester
  • Jake Bromage

    • Laboratory for Laser Energetics, U. of Rochester
  • Dustin H Froula

    • University of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
    • Lab for Laser Energetics
    • Laboratory for Laser Energetics
    • Laboratory for Laser Energetics, University of Rochester