Bremsstrahlung cannon design for shock ignition relevant regime
Year: 2021
Authors: Koester P., Baffigi F., Cristoforetti G., Labate L., Gizzi LA., Baton S., Koenig M., Colaïtis A., Batani D., Casner A., Raffestin D., Tentori A., Trela J., Rousseaux C., Boutoux G., Brygoo S., Jacquet L., Reverdin C., Le Bel E., Le-Deroff L., Theobald W., Shigemori K.
Autors Affiliation: CNR, Ist Nazl Ott, Intense Laser Irradiat Lab, Via G Moruzzi 1, I-56124 Pisa, Italy; Sorbonne Univ, Ecole Polytech, CNRS, UMR 7605,CEA,Lab Utilisat Lasers Intenses,LULI, F-91128 Palaiseau, France; Univ Bordeaux, CNRS, UMR 5107, CEA,Ctr Lasers Intenses & Applicat,CELIA, F-33405 Talence, France; CEA, Direct Applicat Mil, Commissariat Energie Atom & Energies Alternat, DAM, F-91297 Ile De France, Arpajon, France; CEA, CESTA, Direct Applicat Mil,Ctr Etud Sci & Tech Aquitaine, DAM,Commissariat Energie Atom & Energies Alternat, F-33114 Le Barp, France; Univ Rochester, Lab Laser Energet, Rochester, NY 14623 USA; Osaka Univ, Inst Laser Engn, Osaka 5650871, Japan; Univ Bordeaux, CNRS, UMR 5107, CEA,CELIA,Ctr Lasers Intenses & Applicat, F-33405 Talence, France.
Abstract: We report on the optimization of a BremsStrahlung Cannon (BSC) design for the investigation of laser-driven fast electron populations in a shock ignition relevant experimental campaign at the Laser Megajoule-PETawatt Aquitaine Laser facility. In this regime with laser intensities of 1015 W/cm2–1016 W/cm2, fast electrons with energies ≤100 keV are expected to be generated through Stimulated Raman Scattering (SRS) and Two Plasmon Decay (TPD) instabilities. The main purpose of the BSC in our experiment is to identify the contribution to x-ray emission from bremsstrahlung of fast electrons originating from SRS and TPD, with expected temperatures of 40 keV and 95 keV, respectively. Data analysis and reconstruction of the distributions of x-ray photons incident on the BSC are described.
Journal/Review: REVIEW OF SCIENTIFIC INSTRUMENTS
Volume: 92 (1) Pages from: 013501-1 to: 013501-10
More Information: The authors acknowledge the support from the Enabling Research Project EUROfusion (Task Agreement No. ENR-IFE19.CEA-01, Grant Agreement No. 633053) funded under the Horizon 2020-Euratom program. The PETAL laser was designed and constructed by CEA under the financial auspices of Conseil Regional d´Aquitaine, the French Ministry of Research, and the European Union. The CRACC diagnostic was designed and commissioned at the LMJ-PETAL facility as a result of the PETAL+ project coordinated by Universite de Bordeaux and funded by the French Agence Nationale de la Recherche under Grant No. ANR-10-EQPX-42-01 and the PetaPhys project under Grant No. ANR-10-IDEX-03-02. The LMJ-PETAL experiment presented in this article was supported by Association Lasers et Plasmas and by CEA. The views and opinions expressed herein do not necessarily reflect those of the European Commission.KeyWords: Laser-Plasma Interaction, Hot Electron generation, inertial confinement fusionDOI: 10.1063/5.0022030Citations: 9data from “WEB OF SCIENCE” (of Thomson Reuters) are update at: 2024-09-29References taken from IsiWeb of Knowledge: (subscribers only)Connecting to view paper tab on IsiWeb: Click hereConnecting to view citations from IsiWeb: Click here