Shock-tuned cryogenic-deuterium-tritium implosion performance on Omega

  • T. C. Sangster
  • , V. N. Goncharov
  • , R. Betti
  • , T. R. Boehly
  • , D. T. Casey
  • , T. J.B. Collins
  • , R. S. Craxton
  • , J. A. Delettrez
  • , D. H. Edgell
  • , R. Epstein
  • , K. A. Fletcher
  • , J. A. Frenje
  • , Y. Yu Glebov
  • , D. R. Harding
  • , S. X. Hu
  • , I. V. Igumenschev
  • , J. P. Knauer
  • , S. J. Loucks
  • , C. K. Li
  • , J. A. Marozas
  • F. J. Marshall, R. L. McCrory, P. W. McKenty, D. D. Meyerhofer, P. M. Nilson, S. P. Padalino, R. D. Petrasso, P. B. Radha, S. P. Regan, F. H. Seguin, W. Seka, R. W. Short, D. Shvarts, S. Skupsky, V. A. Smalyuk, J. M. Soures, C. Stoeckl, W. Theobald, B. Yaakobi

Research output: Contribution to journalArticlepeer-review

37 Scopus citations

Abstract

Cryogenic-deuterium-tritium (DT) target compression experiments with low-adiabat (α), multiple-shock drive pulses have been performed on the Omega Laser Facility [T. R. Boehly, D. L. Brown, R. S. Craxton, Opt. Commun. 133, 495 (1997)] to demonstrate hydrodynamic-equivalent ignition performance. The multiple-shock drive pulse facilitates experimental shock tuning using an established cone-in-shell target platform [T. R. Boehly, R. Betti, T. R. Boehly, Phys. Plasmas 16, 056301 (2009)]. These shock-tuned drive pulses have been used to implode cryogenic-DT targets with peak implosion velocities of 3× 107cm/s at peak drive intensities of 8× 1014 W/ cm2. During a recent series of α∼2 implosions, one of the two necessary conditions for initiating a thermonuclear burn wave in a DT plasma was achieved: an areal density of approximately 300 mg/ cm2 was inferred using the magnetic recoil spectrometer [J. A. Frenje, C. K. Li, F. H. Śguin, Phys. Plasmas 16, 042704 (2009)]. The other condition-a burn-averaged ion temperature 〈 Tin of 8-10 keV-cannot be achieved on Omega because of the limited laser energy; the kinetic energy of the imploding shell is insufficient to heat the plasma to these temperatures. A 〈 T in of approximately 3.4 keV would be required to demonstrate ignition hydrodynamic equivalence [Betti, Phys. Plasmas17, 058102 (2010)]. The 〈 Tin reached during the recent series of α∼2 implosions was approximately 2 keV, limited primarily by laser-drive and target nonuniformities. Work is underway to improve drive and target symmetry for future experiments.

Original languageEnglish
Article number056312
JournalPhysics of Plasmas
Volume17
Issue number5
DOIs
StatePublished - 1 May 2010
Externally publishedYes

ASJC Scopus subject areas

  • Condensed Matter Physics

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