Imploding Cryogenic Shell Nonuniformity Measurements on OMEGA by Self-Radiography<sub></sub>

ORAL

Abstract

Radiographs of pure DT cryogenic imploding shells will help to validate progress toward ignition-scalable performance of inertial confinement fusion implosions. Imploding cryogenic D2 and DT shells can be radiographed with the core spectral emission, progressively from 1 keV to ≈2 keV, from the deceleration phase through peak compression. Utilizing the distinct spectral dependences of hydrogen continuum emissivity and opacity, shell optical‑thickness variations can be distinguished from core structure. This technique does not require shell additives, as used in previous applications of implosion self-radiography. Demonstrations with simulated data show that this technique is remarkably well suited to cryogenic implosions. Specifically, emission and absorption are well localized to the core and shell, respectively. Also, shell self-backlighting can be used near peak compression, unlike externally backlit radiography, where self-emission is a background signal that overwhelms the backlighter near peak compression.

*This work was supported by the U.S. Department of Energy National Nuclear Security Administration under Award Number DE-NA0001944.

Presenters

  • Reuben Epstein

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

Authors

  • Reuben Epstein

    • Univ of Rochester
    • Laboratory for Laser Energetics, University of Rochester
    • Lab for Laser Energetics
    • Laboratory for Laser Energetics, U. of Rochester
  • Christian Stoeckl

    • Univ of Rochester, Univ of Rochester
    • Univ of Rochester
    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics
    • Laboratory for Laser Energetics U. of Rochester
    • Lab for Laser Energetics
    • University of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
  • Radha Bahukutumbi

    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics U. of Rochester
    • University of Rochester
    • Univ of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
    • Laboratory for Laser Energetics, U. of Rochester, Laboratory for Laser Energetics, U. of Rochester
    • Lab for Laser Energetics, Univ of Rochester
  • Timothy J Collins

    • Univ of Rochester
    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics U. of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
    • Lab for Laser Energetics, Univ of Rochester
  • Patrick W McKenty

    • University of Rochester Laboratory for Laser Energetics
    • Univ of Rochester
    • Laboratory for Laser Energetics U. of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
  • Duc M Cao

    • Lab for Laser Energetics
    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics U. of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
  • Rahul C Shah

    • Lab for Laser Energetics
    • Laboratory for Laser Energetics
    • Laboratory for Laser Energetics, University of Rochester
    • Laboratory for Laser Energetics, U. of Rochester
    • Lab for Laser Energetics, Univ of Rochester
  • Dylan T Cliche

    • Univ of Nevada - Reno
    • Univ of Nevada - Reno, Los Alamos National Laboratory
  • Roberto Claudio Mancini

    • Univ of Nevada - Reno
    • University of Nevada - Reno
    • Physics Department, University of Nevada, Reno, Nevada