Communications Physics (Jun 2023)

Probing strong-field QED in beam-plasma collisions

  • Aimé Matheron,
  • Pablo San Miguel Claveria,
  • Robert Ariniello,
  • Henrik Ekerfelt,
  • Frederico Fiuza,
  • Spencer Gessner,
  • Max F. Gilljohann,
  • Mark J. Hogan,
  • Christoph H. Keitel,
  • Alexander Knetsch,
  • Mike Litos,
  • Yuliia Mankovska,
  • Samuele Montefiori,
  • Zan Nie,
  • Brendan O’Shea,
  • J. Ryan Peterson,
  • Doug Storey,
  • Yipeng Wu,
  • Xinlu Xu,
  • Viktoriia Zakharova,
  • Xavier Davoine,
  • Laurent Gremillet,
  • Matteo Tamburini,
  • Sébastien Corde

DOI
https://doi.org/10.1038/s42005-023-01263-4
Journal volume & issue
Vol. 6, no. 1
pp. 1 – 9

Abstract

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Abstract Ongoing progress in laser and accelerator technology opens new possibilities in high-field science, notably to investigate the largely unexplored strong-field quantum electrodynamics (SFQED) regime where electron-positron pairs can be created directly from light-matter or even light-vacuum interactions. Laserless strategies such as beam-beam collisions have also been proposed to access the nonperturbative limit of SFQED. Here we report on a concept to probe SFQED by harnessing the interaction between a high-charge, ultrarelativistic electron beam and a solid conducting target. When impinging onto the target surface, the beam self fields are reflected, partly or fully, depending on the beam shape; in the rest frame of the beam electrons, these fields can exceed the Schwinger field, thus triggering SFQED effects such as quantum nonlinear inverse Compton scattering and nonlinear Breit-Wheeler electron-positron pair creation. Through reduced modeling and kinetic numerical simulations, we show that this single-beam setup can achieve interaction conditions similar to those envisioned in beam-beam collisions, but in a simpler and more controllable way owing to the automatic overlap of the beam and driving fields. This scheme thus eases the way to precision studies of SFQED and is also a promising milestone towards laserless studies of nonperturbative SFQED.