Collective stimulated Brillouin backscatter

dc.creatorLushnikov, Pavel M.
dc.creatorRose, Harvey A.
dc.date2007-10-02
dc.date.accessioned2026-07-07T08:33:40Z
dc.date.available2026-07-07T08:33:40Z
dc.descriptionWe develop the statistical theory of the stimulated Brillouin backscatter (BSBS) instability of a spatially and temporally partially incoherent laser beam for laser fusion relevant plasma. We find a new regime of BSBS which has a much larger threshold than the classical threshold of a coherent beam in long-scale-length laser fusion plasma. Instability is collective because it does not depend on the dynamics of isolated speckles of laser intensity, but rather depends on averaged beam intensity. We identify convective and absolute instability regimes. Well above the incoherent threshold the coherent instability growth rate is recovered. The threshold of convective instability is inside the typical parameter region of National Ignition Facility (NIF) designs although current NIF bandwidth is not large enough to insure dominance of collective instability and suggests lower instability threshold due to speckle contribution. In contrast, we estimate that the bandwidth of KrF-laser-based fusion systems would be large enough.
dc.description4 pages, 3 figures
dc.identifierhttps://arxiv.org/abs/0710.0634
dc.identifierhttp://arxiv.org/abs/0710.0634
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/139209
dc.subjectPlasma Physics
dc.titleCollective stimulated Brillouin backscatter
dc.typetext

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