Abstract
We study the trident process in laser pulses. We provide exact numerical results for all contributions, including the difficult exchange term. We show that all terms are in general important for a short pulse. For a long pulse, we identify a term that gives the dominant contribution even if the intensity is only moderately high, , which is an experimentally important regime where the standard locally constant field (LCF) approximation cannot be used. We show that the spectrum has a richer structure at , compared to the LCF regime . We study the convergence to LCF as increases and how this convergence depends on the momentum of the initial electron. We also identify the terms that dominate at high energy.
- Received 9 January 2020
- Revised 3 February 2020
- Accepted 11 February 2020
DOI:https://doi.org/10.1103/PhysRevD.101.056017
Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.
Published by the American Physical Society