Cryogenic tritium-hydrogen-deuterium and deuterium-tritium layer implosions with high density carbon ablators in near-vacuum hohlraums

  • N. B. Meezan
  • , L. F. Berzak Hopkins
  • , S. Le Pape
  • , L. Divol
  • , A. J. Mackinnon
  • , T. Döppner
  • , D. D. Ho
  • , O. S. Jones
  • , S. F. Khan
  • , T. Ma
  • , J. L. Milovich
  • , A. E. Pak
  • , J. S. Ross
  • , C. A. Thomas
  • , L. R. Benedetti
  • , D. K. Bradley
  • , P. M. Celliers
  • , D. S. Clark
  • , J. E. Field
  • , S. W. Haan
  • N. Izumi, G. A. Kyrala, J. D. Moody, P. K. Patel, J. E. Ralph, J. R. Rygg, S. M. Sepke, B. K. Spears, R. Tommasini, R. P.J. Town, J. Biener, R. M. Bionta, E. J. Bond, J. A. Caggiano, M. J. Eckart, M. Gatu Johnson, G. P. Grim, A. V. Hamza, E. P. Hartouni, R. Hatarik, D. E. Hoover, J. D. Kilkenny, B. J. Kozioziemski, J. J. Kroll, J. M. McNaney, A. Nikroo, D. B. Sayre, M. Stadermann, C. Wild, B. E. Yoxall, O. L. Landen, W. W. Hsing, M. J. Edwards

Research output: Contribution to journalArticlepeer-review

Abstract

High Density Carbon (or diamond) is a promising ablator material for use in near-vacuum hohlraums, as its high density allows for ignition designs with laser pulse durations of <10-ns. A series of Inertial Confinement Fusion (ICF) experiments in 2013 on the National Ignition Facility [Moses et al., Phys. Plasmas 16, 041006 (2009)] culminated in a deuterium-tritium (DT) layered implosion driven by a 6.8-ns, 2-shock laser pulse. This paper describes these experiments and comparisons with ICF design code simulations. Backlit radiography of a tritium-hydrogen-deuterium (THD) layered capsule demonstrated an ablator implosion velocity of 385-km/s with a slightly oblate hot spot shape. Other diagnostics suggested an asymmetric compressed fuel layer. A streak camera-based hot spot self-emission diagnostic (SPIDER) showed a double-peaked history of the capsule self-emission. Simulations suggest that this is a signature of low quality hot spot formation. Changes to the laser pulse and pointing for a subsequent DT implosion resulted in a higher temperature, prolate hot spot and a thermonuclear yield of 1.8-×-1015 neutrons, 40% of the 1D simulated yield.

Original languageEnglish
Article number062703
JournalPhysics of Plasmas
Volume22
Issue number6
DOIs
Publication statusPublished - 1 Jun 2015
Externally publishedYes

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