Breit-Wheeler process in very short electromagnetic pulses

Abstract

The generalized Breit-Wheeler process, i.e., the emission of ${e}^{+}{e}^{\ensuremath{-}}$ pairs off a probe photon propagating through a polarized short-pulsed electromagnetic (e.g., laser) wave field, is analyzed. We show that the production probability is determined by the interplay of two dynamical effects. The first one is related to the shape and duration of the pulse and the second one is the nonlinear dynamics of the interaction of ${e}^{\ifmmode\pm\else\textpm\fi{}}$ with the strong electromagnetic field. The first effect manifests itself most clearly in the weak-field regime, where the small field intensity is compensated by the rapid variation of the electromagnetic field in a limited space-time region, which intensifies the few-photon events and can enhance the production probability by orders of magnitude compared to an infinitely long pulse. Therefore, short pulses may be considered as a powerful amplifier. The nonlinear dynamics in the multiphoton Breit-Wheeler regime plays a decisive role at large field intensities, where effects of the pulse shape and duration are less important. In the transition regime, both effects must be taken into account simultaneously. We provide suitable expressions for the ${e}^{+}{e}^{\ensuremath{-}}$ production probability for kinematic regions which can be used in transport codes.