Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session UP11: Poster Session VIII: MST; DIII-D Tokamak; SPARC, C-Mod, and High Field Tokamaks; HBT-EP; Transport and LPI in ICF Plasmas, Hydrodynamic Instability; HEDP Posters; Space and Astrophysical Plasmas (2:00pm-5:00pm)
Thursday, November 8, 2018
OCC
Room: Exhibit Hall A1&A
Abstract ID: BAPS.2018.DPP.UP11.103
Abstract: UP11.00103 : Impact of laser bandwidth on SRS in ICF plasmas*
Presenter:
Andrew J Schmitt
(Naval Research Lab)
Authors:
Andrew J Schmitt
(Naval Research Lab)
John G Shaw
(LLE/University of Rochester)
Jason F Myatt
(Univ of Alberta)
Laurance J Suter
(Lawrence Livermore Natl Lab)
In laser driven ICF plasmas, higher pressures are used to drive more hydrodynamically stable implosions, but the pressure (intensity) is limited by laser plasma instabilities (LPI) like stimulated Raman scattering (SRS). Bandwidth is known to stabilize or mitigate LPIs particularly when it is comparable to or greater than the growth-time of the instability1. Because of their faster growth rate, plasmon-based instabilities like SRS need more bandwidth for suppression than ion-acoustic instabilities like SBS or filamentation. However, relatively large bandwidths (Δν > 2 THz) can be impressed on an otherwise narrow-bandwidth laser using stimulated rotatational Raman scattering (SRRS) in gas2. Here we use the LPSE3 code to investigate the impact of SRRS-generated bandwidths on SRS in laser-driven plasmas and report on the results.
1. J.J. Thomson, Nucl.Fusion 15, 237 (1975); S.P. Obenschain and N.C. Luhmann, Appl.Phys.Lett. 30, 452 (1977).
2. J.L. Weaver, et al., Appl.Opt. 56, 8618 (2017).
3. A.V. Maximov et. al, BAPS 62, 75 (2017); J.W. Bates et al., Phys Rev. E 97, 061202 (2018)
*supported by US DoE/NNSA
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.UP11.103
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