Cryogenic-target performance and implosion physics studies on OMEGA
Author(s) -
V. A. Smalyuk,
R. Betti,
T. R. Boehly,
R. S. Craxton,
J. A. Delettrez,
D. H. Edgell,
V. Yu. Glebov,
V. N. Goncharov,
D. R. Harding,
S. X. Hu,
J. P. Knauer,
F. J. Marshall,
R. L. McCrory,
P. W. McKenty,
D. D. Meyerhofer,
P. B. Radha,
S. P. Regan,
T. C. Sangster,
W. Seka,
R. W. Short,
D. Shvarts,
S. Skupsky,
J. M. Soures,
C. Stöeckl,
B. Yaakobi,
J. A. Frenje,
C. K. Li,
R. D. Petrasso,
F. H. Séguin
Publication year - 2009
Publication title -
physics of plasmas
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.75
H-Index - 160
eISSN - 1089-7674
pISSN - 1070-664X
DOI - 10.1063/1.3078102
Subject(s) - implosion , physics , hohlraum , rayleigh–taylor instability , inertial confinement fusion , laser , shock wave , national ignition facility , atomic physics , shock (circulatory) , omega , plasma , electron , instability , intensity (physics) , z pinch , optics , nuclear physics , mechanics , medicine , quantum mechanics
Recent progress in direct-drive cryogenic implosions on the OMEGA Laser Facility [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)] is reviewed. Ignition-relevant areal densities of ~200 mg/cm^2 in cryogenic D2 implosions with peak laser-drive intensities of ~5 x 10^14 W/cm^2 were previously reported [T. C. Sangster et al., Phys. Rev. Lett. 100, 185006 (2008)]. The laser intensity is increased to ~10^15 W/cm^2 to demonstrate ignition-relevant implosion velocities of 3–4 x 10^7 cm/ s, providing an understanding of the relevant target physics. Planar-target acceleration experiments show the importance of the nonlocal electron-thermal-transport effects for modeling the laser drive. Nonlocal and hot-electron preheat is observed to stabilize the Rayleigh–Taylor growth at a peak drive intensity of ~10^15 W/cm^2. The shell preheat caused by hot electrons generated by two-plasmon-decay instability was reduced by using Si-doped ablators. The measured compressibility of planar plastic targets driven with high-compression shaped pulses agrees well with one-dimensional simulations at these intensities. Shock mistiming has contributed to compression degradation of recent cryogenic implosions driven with continuous pulses. Multiple-picket (shock-wave) target designs make it possible for a more robust tuning of the shock-wave arrival times. Cryogenic implosions driven with double-picket pulses demonstrate somewhat improved compression performance at a peak drive intensity of ~10^15 W/cm^2
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