We show how to use a worldline-instanton formalism to calculate, to leading order in the weak-field expansion, the momentum spectrum of nonlinear Breit-Wheeler pair production in fields that depend on time and one spatial coordinate. We find a nontrivial dependence on the width, λ, of the photon wave packet, and the existence of a critical point λc. For λ<λc and a field with one peak, the spectrum has one peak where the electron and positron have the same energy. For λ>λc this splits into two peaks. We calculate a high-energy (Ω≫1) expansion, which to leading order agrees with the results obtained by replacing the spacetime field with a plane wave and using the well-known Volkov solutions. We also calculate an expansion for Ω∼a0≫1, where the field is strong enough to significantly bend the trajectories of the fermions despite Ω≫1. Published by the American Physical Society 2024
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