Radiation-dominated injection of positrons generated by the nonlinear Breit-Wheeler process into a plasma channel

TL;DR

This paper investigates the nonlinear Breit-Wheeler process for positron generation and injection into plasma channels under ultra-high laser intensities, highlighting radiation reaction effects and potential for positron acceleration.

Contribution

It demonstrates the critical role of radiation reaction in positron injection and shows how ultra-high laser intensities enable efficient positron injection and acceleration in plasma channels.

Findings

Positron injection efficiency increases rapidly above 2.2x10^23 W/cm^2.

Radiation reaction suppresses initial transverse momentum of positrons.

Laser-driven plasma channels can double positron energy through direct acceleration.

Abstract

Plasma acceleration is considered a prospective technology for building a compact multi-TeV electron-positron collider in the future. The challenge of this endeavor is greater for positrons than for the electrons because usually the self-generated fields from laser-plasma interaction are not well-suited for positron focusing and on-axis guiding. In addition, an external positron source is required, while electrons are naturally available in the plasma. Here, we study electron-positron pair generation by an orthogonal collision of a multi-PW laser pulse and a GeV electron beam by the nonlinear Breit-Wheeler process. We studied conditions favorable for positron deflection in the direction of the laser pulse propagation, which favors injection into the plasma for further acceleration. We demonstrate using the OSIRIS particle-in-cell framework that the radiation reaction triggered by ultra-high laser intensity plays a crucial role in the positron injection. It provides a suppression of the initial transverse momentum gained by the positrons from the Breit-Wheeler process. For the parameters used in this work, the intensity of at least 2.2x1023 W/cm2 is needed in order to inject more than 1% of positrons created. Above this threshold, the percentage of injected positrons rapidly increases with intensity. Moreover, subsequent direct laser acceleration of positrons in a plasma channel, using the same laser pulse that created them, can ensure a boost of the final positron energy by a factor of two. The positron focusing and guiding on the axis is provided by significant electron beam loading that changes the internal structure of the channel fields.