Numéro |
J. Phys. IV France
Volume 133, June 2006
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Page(s) | 233 - 235 | |
DOI | https://doi.org/10.1051/jp4:2006133047 | |
Publié en ligne | 16 juin 2006 |
J.-C. Gauthier, et al.
J. Phys. IV France 133 (2006) 233-235
DOI: 10.1051/jp4:2006133047
Polar direct drive - Ignition at 1 MJ
S. Skupsky, R.S. Craxton, F.J. Marshall, R. Betti, T.J.B. Collins, R.Epstein, V.N. Goncharov, I.V. Igumenshchev, J.A. Marozas, P.W. McKenty, P.B. Radha, J.D. Kilkenny, D.D. Meyerhofer, T.C. Sangster and R.L. McCroryLaboratory for Laser Energetics, University of Rochester, 250 East River Road, Rochester, NY 14623, USA
Abstract
Target designs to achieve direct-drive ignition on the
NIF using the x-ray-drive beam configuration are examined. This approach,
known as polar direct drive (PDD), achieves the required irradiation
uniformity by repointing some of the beams toward the target equator, and by
increasing the laser intensity at the equator to compensate for the reduced
laser coupling from oblique irradiation. Techniques to increase the
equatorial intensity can include using phase plates that produce elliptical
spot shapes, increasing the power in beams directed toward the equator, and
using a ring offset from the equator to redirect rays toward the target
normal. The requirements for beam pointing, power balance, single-beam
smoothing, and inner-ice-surface roughness are examined. Designs with an
incident laser energy of 1.0 MJ are presented. The simulations use the 2-D
hydrocode DRACO with 3-D ray trace to model the laser irradiation and Monte Carlo
alpha particle transport to model the thermonuclear burn.
© EDP Sciences 2006