• Open Access

Effects of hydrogen concentration in ablator material on stimulated Raman scattering, two-plasmon decay, and hot electrons for direct-drive inertial confinement fusion

K. Kawasaki, G. Cristoforetti, T. Idesaka, Y. Hironaka, D. Tanaka, D. Batani, S. Fujioka, L. A. Gizzi, M. Hata, T. Johzaki, K. Katagiri, R. Kodama, S. Matsuo, H. Nagatomo, Ph. Nicolai, N. Ozaki, Y. Sentoku, R. Takizawa, A. Yogo, H. Yamada, and K. Shigemori
Phys. Rev. Research 5, 033051 – Published 25 July 2023

Abstract

Laser plasma instabilities, such as stimulated Raman scattering (SRS) and two-plasmon decay (TPD), are basic phenomena in intense laser science and applications. In direct-drive inertial confinement fusion (ICF) where a fuel capsule is imploded by high-power lasers, SRS and TPD are generally problematic because hot electrons (HEs) generated by SRS and TPD cause fuel preheating, whereas HEs with acceptable energy are expected to contribute to ablation pressure enhancement. In all cases, it is necessary to clarify the occurrence of SRS, TPD, and subsequent HE generation. The ablator of a fuel capsule in direct-drive ICF typically consists of carbon with a variable amount of hydrogen (H). We investigated the H effects in the ablator on SRS, TPD, and HEs under direct-drive ICF conditions at the GEKKO laser facility in planer geometry. The experimental results showed an increase in SRS, TPD, and HEs when H was present in the ablator. The analysis indicated that the variations in plasma inhomogeneity and plasma temperature obtained by H addition were insufficient to explain the observed results. Thus, the enhancement is mainly attributed to the high ion acoustic wave damping driven by the H ions into the plasmas, suggesting that Langmuir decay instability caused SRS saturation, whereas other mechanisms, such as cavitation, could overwhelm the TPD saturation. These results suggest that a suitable choice of H concentration in the ablator is critical for mitigating and controlling the extent of SRS, TPD, and HEs to achieve robust and efficient implosion in direct-drive ICF.

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  • Received 6 March 2023
  • Accepted 12 July 2023

DOI:https://doi.org/10.1103/PhysRevResearch.5.033051

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.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Plasma Physics

Authors & Affiliations

K. Kawasaki1,*, G. Cristoforetti2, T. Idesaka1, Y. Hironaka1, D. Tanaka1, D. Batani3, S. Fujioka1, L. A. Gizzi2, M. Hata4, T. Johzaki5, K. Katagiri6, R. Kodama1,6, S. Matsuo1, H. Nagatomo1, Ph. Nicolai3, N. Ozaki1,6, Y. Sentoku1, R. Takizawa1, A. Yogo1, H. Yamada7, and K. Shigemori1

  • 1Institute of Laser Engineering, Osaka University, 2-6 Yamadaoka, Suita, Osaka 565-0871, Japan
  • 2Intense Laser Irradiation Laboratory, INO-CNR, 56124 Pisa, Italy
  • 3Centre Lasers Intenses et Applications, CELIA, University Bordeaux CEA-CNRS, UMR 5107, F-33405 Talence, France
  • 4National Institute for Fusion Science, 332-6 Oroshicho, Toki, Gifu 509-5202, Japan
  • 5Graduate School of Engineering, Hiroshima University, 1-4-1 Kagamiyama, Higashi-Hiroshima, Hiroshima 739-8527, Japan
  • 6Graduate School of Engineering, Osaka University, 2-6 Yamadaoka, Suita, Osaka 565-0871, Japan
  • 7Diamond Material Team, Advanced Power Electronics Research Center, National Institute of Advanced Industrial Science and Technology, 1-8-31 Midorigaoka, Ikeda, Osaka 563-0026, Japan

  • *u710983e@ecs.osaka-u.ac.jp

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Vol. 5, Iss. 3 — July - September 2023

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