54th Annual Meeting of the APS Division of Plasma Physics
Volume 57, Number 12
Monday–Friday, October 29–November 2 2012;
Providence, Rhode Island
Session YI2: Laser-plasma Interactions, Kinetic Effects and Invited Post-deadline
9:30 AM–12:30 PM,
Friday, November 2, 2012
Room: Ballroom DE
Chair: Andrew Schmitt, Naval Research Laboratory
Abstract ID: BAPS.2012.DPP.YI2.2
Abstract: YI2.00002 : Experimental validation of the two-plasmon-decay common-wave process
10:00 AM–10:30 AM
Preview Abstract
Abstract
Author:
D.T. Michel
(Laboratory for Laser Energetics, University of Rochester)
Direct-drive inertial confinement fusion requires multiple overlapping laser beams that can drive the two-plasmon-decay (TPD) instability. When multiple overlapping laser beams with polarization smoothing are used, the total energy in TPD-generated hot electrons was shown to scale with the overlapped intensity.\footnote{C. Stoeckl\textit{ et al.}, Phys. Rev. Lett. \textbf{90}, 235002 (2003).} This scaling would not be expected if the beams drive the TPD independently according to the single-plane wave growth rates. Experiments were conducted on OMEGA EP, in large-scale-length plasmas, to validate the common-wave process, where the total energy in hot electrons is measured to be similar when one or two polarized beams are used at the same overlapped intensity and significantly reduced when four beams with the same overlapped intensity are used.\footnote{D. T. Michel \textit{et al}., ``Experimental Validation of the Two-Plasmon-Decay Common-Wave Process,'' submitted to Physical Review
Letters.} A theoretical model of the common-wave process shows that multiple laser beams can share an electron-plasma wave in the region bisecting the electromagnetic wave vectors. For two beams, this region defines a plane; for four beams, it defines a line. In this region, the convective gain of the dominant mode is proportional to the overlapped intensity and a geometric factor. When the TPD instability is saturated, the hot-electron temperature increases rapidly (25 keV to 90 keV), consistent with Zakharov simulations.\footnote{D. H. Froula\textit{ et al.}, Phys. Rev. Lett. \textbf{108}, 165003 (2012).} This work was supported by the U.S. Department of Energy Office of Inertial Confinement Fusion under Cooperative Agreement No. DE-FC52-08NA28302.\\[4pt]
In collaboration with A. V. Maximov, R. W. Short, J. F. Myatt, W. Seka, J. A. Delettrez, R. Follett, S. X. Hu, A. A. Solodov, C. Stoeckl, B. Yaakobi, and D. H. Froula (Laboratory for Laser Energetics, Univ. of Rochester).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2012.DPP.YI2.2