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

0584067 - ÚFP 2024 RIV US eng J - Článek v odborném periodiku
Mašlárová, Dominika - Martinez, B. - Vranic, M.
Radiation-dominated injection of positrons generated by the nonlinear Breit-Wheeler process into a plasma channel.
Physics of Plasmas. Roč. 30, č. 9 (2023), č. článku 093107. ISSN 1070-664X. E-ISSN 1089-7674
Grant CEP: GA MŠMT(CZ) EF18_053/0016925; GA MŠMT EF16_019/0000778
Výzkumná infrastruktura: e-INFRA CZ - 90140
Institucionální podpora: RVO:61389021
Klíčová slova: Breit-Wheeler process * plasma channel * positron
Obor OECD: Fluids and plasma physics (including surface physics)
Impakt faktor: 2.2, rok: 2022
Způsob publikování: Omezený přístup
https://pubs.aip.org/aip/pop/article/30/9/093107/2913099/Radiation-dominated-injection-of-positrons

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 2.2 × 10 23 W / cm 2 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.
Trvalý link: https://hdl.handle.net/11104/0352074