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Extra resources for Inertial Confinement Fusion [quarterly rpt Apr-Jun 1998]
E. Max, Phys. Fluids 1, 74 (1976); M. V. Goldman, K. Rypdal, and B. Hafizi, ibid. 23, 945 (1980); J. J. Rasmussen and K. Rypdal, Phys. Scr. 3, 481 (1986). W. L. Kruer and J. H. Hammer, Comments Plasma Phys. Control. Fusion 18, 85 (1997). -Z. Sun, E. Ott, Y. C. Lee, and P. Guzdar, Phys. Fluids 30, 526 (1987); M. D. Feit, J. C. Garrison, and A. M. Rubenchik, Phys. Rev. E 56, 2394 (1997). D. W. , Phys. Rev. Lett. 54, 558 (1985); W. B. , ibid. 60, 1298 (1988); K. C. Tzeng, W. B. Mori, and C. D. Decker, ibid.
Ibid. 60, 1298 (1988); K. C. Tzeng, W. B. Mori, and C. D. Decker, ibid. 76, 3332 (1996). 129 NOVA/BEAMLET/NIF UPDATES APRILÐJUNE 1998 R. Ehrlich/P. Wegner/S. Kumpan Nova Operations Nova Operations performed 229 experiments during this quarter. These experiments supported efforts in ICF, Defense Sciences, university collaborations, Laser Science, and Nova facility maintenance. 5 hours of overlap between shifts. m. m. This will allow the operations group to achieve the goal of 900 experiments in FY 1998.
Laser-Beam Deflection by Transverse Plasma Flow UCRL-LR-105821-98-3 [(∂t + u∂x + ν)(∂t + u∂x ) − Cs2∇2⊥ ]δn = 1 2 2 2 Cs (v0 ve ) ∇ 2⊥ ψ . 4 (1b) Here, ψ is the light-wave vector potential scaled to its peak value, δn is the fractional density perturbation, k0 is the laser wave number, ωpe is the electron-plasma frequency, c is the speed of light, ν is the ion damping rate, u is the transverse plasma flow, Cs is the sound speed, v0 is the electron quiver velocity in the peak light wave electric field, and ve is the electron thermal velocity.