29 June 2026 to 3 July 2026
EICC, Edinburgh
Europe/London timezone

Parametric study of Coherent Transition Radiation characteristics across underdense to overdense plasma densities

Not scheduled
20m
EICC, Edinburgh

EICC, Edinburgh

150 Morrison St, Edinburgh EH3 8EE
Poster Presentation Laser-plasma Acceleration of Particles and Plasma-based Radiation Sources (BPIF)

Description

Coherent Transition Radiation (CTR) is a primary mechanism for generating high-energy electromagnetic pulses (EMP) in ultra-high intensity laser-plasma interactions [1], reaching sub-Joule to Joule-level energies in the THz range [2,3]. Its characteristics are highly sensitive to the longitudinal and transverse properties of the laser-accelerated electron bunches as they cross the plasma-vacuum interface and, therefore, to the underlying acceleration mechanism.
In this work, we employ two-dimensional particle-in-cell (PIC) simulations using the code CALDER [4], which solves the relativistic Vlasov-Maxwell equations, to perform a parametric study on CTR emission as a function of the target density ranging from underdense ($< 0.01 \, n_{cr}$) to overdense ($\sim 30 \, n_{cr}$) plasma densities. Focusing on an experimentally feasible design with high-repetition-rate gas targets and ultra-short (few- to multi-cycle), Joule-class laser pulses [5], we identify through angular and spectral features that the radiation carries the imprint of the underlying acceleration mechanism — e.g. wakefield acceleration in the blowout regime [6] or electron acceleration in laser-solid interactions [7]. We characterize the transition between the different acceleration mechanisms and find good agreement with theoretical predictions on the impact on the THz yield and spectral distribution.
[1] A. Poyé et al., Phys. Rev. E 91, 043106 (2015).
[2] G. Liao et al., Phys. Rev. X 10, 031062 (2020).
[3] G. Bruhaug et al., Opt. Lett. 49, 1737 (2024).
[4] E. Lefebvre et al., Nucl. Fusion 43, 629 (2003).
[5] M. O. Cernaianu et al., Matter Radiat. Extremes 10, 027204 (2025).
[6] J. Déchard et al., Phys. Rev. Lett. 120, 144801 (2018).
[7] E. Denoual et al., Phys. Rev. E 108, 065211 (2023).

Authors

Camilla Willim (Centre des Lasers Intenses et Applications, Université de Bordeaux-CNRS-CEA, F-33405 Talence Cedex, France) Émilien Denoual (CEA, DAM, DIF, F-91297 Arpajon, France; Université Paris-Saclay, CEA, LMCE, F-91680 Bruyères-le-Châtel, France) Xavier Davoine (CEA, DAM, DIF, F-91297 Arpajon, France; Université Paris-Saclay, CEA, LMCE, F-91680 Bruyères-le-Châtel, France) Laurent Gremillet (CEA, DAM, DIF, F-91297 Arpajon, France; Université Paris-Saclay, CEA, LMCE, F-91680 Bruyères-le-Châtel, France) Emmanuel d’Humières (CELIA, Université de Bordeaux–CNRS–CEA, UMR 5107, Talence F-33405, France) Luc Bergé (CELIA, Université de Bordeaux–CNRS–CEA, UMR 5107, Talence F-33405, France)

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