Studies of kinetic effects in shock-driven implosions using a comprehensive set of x-ray and nuclear diagnostics at OMEGA

ORAL

Abstract

In thin-glass, shock-driven implosions, a strong shock propagates through the plasma during the early phase of implosion.  This strong shock heats the low-density material causing the ions’ mean-free path to be larger than the hydrodynamic length scale. Previous studies demonstrated substantial yield degradation as the fill pressure was decreased. Radiation-hydrodynamic simulations using empirically-tuned ion kinetic models [M. J. Rosenberg et al. PRL 2014] and simulations solving the Vlasov-Fokker-Plank equations for the ions [O. Larroche et al. PoP 2016] reproduce the yield-degradation trend. Both simulation methods predict the dominant mechanism responsible for the yield degradation is kinetic ion-diffusion, which interchanges D3He gas with the glass shell. We report on a set of x-ray measurements from a series of implosions with varied D3He gas fill. The measurements show increased x-ray emission as the D3He gas-fill pressure decreases. In addition, x-ray images in multiple energy bands show a transition from a shell-like emission to a center-like emission structure as the gas-fill pressure decreases. Both observations support the prediction of a partial interchange between the glass and D3He due to the long mean-free paths. These x-ray measurements provide an additional constraint for the kinetic modeling of ICF implosions. Results are compared to iFP, xRage, and ARES simulation codes.

*This work was supported in part by the U.S. DOE, the MIT/NNSA CoE, NLUF, LLE, LLNL, and DOE NNSA SSGF.

Presenters

  • Patrick J Adrian

    • Massachusetts Institute of Technology (MIT)
    • Massachusetts Institute of Technology
    • Massachusetts Institute of Technology MIT
    • Massachusetts Institute of Technology MI

Authors

  • Patrick J Adrian

    • Massachusetts Institute of Technology (MIT)
    • Massachusetts Institute of Technology
    • Massachusetts Institute of Technology MIT
    • Massachusetts Institute of Technology MI
  • Johan A Frenje

    • Massachusetts Institute of Technology MIT
    • MIT PSFC
    • Massachusetts Institute of Technology (MIT)
  • Benjamin Bachmann

    • Lawrence Livermore Natl Lab
    • LLNL
  • Vladimir Y Glebov

    • Lab for Laser Energetics
    • University of Rochester
    • Laboratory for Laser Energetics, University of Rochester
  • Maria Gatu-Johnson

    • MIT Plasma Science and Fusion Center
    • MIT PSFC
    • MIT
    • Massachusetts Institute of Technology (MIT)
    • Massachusetts Institute of Technology MI
  • Neel Kabadi

    • Massachusetts Institute of Technology
    • MIT
    • Massachusetts Institute of Technology MIT
    • Massachusetts Institute of Technology (MIT)
  • Justin H Kunimune

    • Massachusetts Institute of Technology
    • Massachusetts Institute of Technology MI
  • Chikang Li

    • Massachusetts Institute of Technology MIT
    • MIT
  • Sean P Regan

    • Laboratory for Laser Energetics, University of Rochester
    • University of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
    • Laboratory for Laser Energetics
    • Lab for Laser Energetics
  • Fredrick H Seguin

    • Massachusetts Institute of Technology MIT
  • Christian Stoeckl

    • University of Rochester
    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
    • Lab for Laser Energetics
    • Laboratory for Laser Energetics
  • Graeme Sutcliffe

    • Massachusetts Institute of Technology
    • Massachusetts Institute of Technology MIT
    • Massachusetts Institute of Technology MI
  • Jacob A Pearcy

    • Massachusetts Institute of Technology
    • Massachusetts Institute of Technology MIT
  • Richard Petrasso

    • Massachusetts Institute of Technology MIT
    • MIT