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Dependence of Hot Electron Generation on Hydrogen Concentration of Target Materials for Shock Ignition Scheme of Direct-Drive Inertial Confinement Fusion

ORAL

Abstract

Shock ignition (SI) scheme is one of promising approaches for controlled nuclear fusion where a fuel capsule is imploded in two stages: compression stage and ignition stage, which requires more than 30 TPa of ultrahigh pressure creation by high intensity spike pulse irradiation in the ignition stage. In spike pulse (1016 W/cm2), hot electrons are produced by parametric instabilities and hot electron assisted laser ablation is considered. Although hot electrons should be avoided in terms of fuel preheating in compression stage, it is pointed out that hot electrons enhance ablation pressure in the SI scheme since compressed capsule in ignition stage already has high arial density, which indicates the control of hot electrons is crucial. We aim to control hot electron generation by target-based approach. Ablator materials of different H concentration: polyethylene (CH2, 66 at%), polystyrene (CH, 50 at%), and diamond (C, 0 at%) were explored in the SI relevant conditions at GEKKO-XII laser facility, where a planer target can be irradiated by pseudo-single beam bundled 12 laser beams. In the presentation, we will show the experimental results for hot electron characterization with simulation calculations which explain hot electron generation increases with increasing H concentration.

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Publication: K. Kawasaki et al, "The role of hot electrons on ultrahigh pressure generation relevant to shock ignition conditions", High Energy Density Physics 37, 100892 (2020)<br>T. Tamagawa et al, "Development of an experimental platform for the investigation of laser–plasma interaction in conditions relevant to shock ignition regime", Review of Scientific Instruments 93, 063505 (2022)

Presenters

  • Koki Kawasaki

    Osaka Univ, Institute of Laser Engineering, Osaka University

Authors

  • Koki Kawasaki

    Osaka Univ, Institute of Laser Engineering, Osaka University

  • Syunnosuke Matsuo

    Institute of Laser Engineering, Osaka university

  • Tomoyuki Idesaka

    Institute of Laser Engineering, Osaka university

  • Yoichiro Hironaka

    Institute of Laser Engineering, Osaka university

  • Daisuke Tanaka

    Institute of Laser Engineering, Osaka university

  • Hideo Nagatomo

    Institute of Laser Engineering, Osaka university

  • Masyasu Hata

    National Institutes for Quantum Science and Technology

  • Ryunosuke Takizawa

    Osaka University, Institute of Laser Engineering, Osaka university

  • Shinsuke Fujioka

    Institute of Laser Engineering, Osaka university

  • Akifumi Yogo

    Institute of Laser Engineering, Osaka university

  • Yasuhiko Sentoku

    Osaka Univ, Institute of Laser Engineering, Osaka university

  • Yasunobu Arikawa

    Institute of Laser Engineering, Osaka university

  • Norimasa Ozaki

    Osaka Univ, Graduate school of engneering, Osaka university

  • ryosuke Kodama

    Institute of Laser Engineering, Osaka university

  • Kento Katagiri

    Osaka Univ, Graduate school of engineering, Osaka university

  • Kunioki Mima

    Osaka Univ, Institute of Laser Engineering, Osaka university

  • Yoshitaka Mori

    The Graduate School for the Creation of New Photonics Industries

  • Tomoyuki Jozaki

    Graduate School of Engineering, Hiroshima University

  • Hideaki Yamada

    National Institute of Advanced Industrial Science and Technology

  • Dimitri Batani

    CELIA, University Bordeaux, University of Bordeaux, France

  • Gabriele Cristoforetti

    Intense Laser Irradiation Laboratory, INO-CNR

  • Keisuke Shigemori

    Osaka Univ, Institute of Laser Engineering, Osaka university