4.4 Article

Experimental investigation of the stimulated Brillouin scattering growth and saturation at 526 and 351 nm for direct drive and shock ignition

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PHYSICS OF PLASMAS
卷 19, 期 1, 页码 -

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AIP Publishing
DOI: 10.1063/1.3677256

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  1. Agence Nationale de Recherche [ANR-07-BLAN-0004]
  2. Agence Nationale de la Recherche (ANR) [ANR-07-BLAN-0004] Funding Source: Agence Nationale de la Recherche (ANR)

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We have designed experiments to study the effect of the laser wavelength (0.527 versus 0.351 mu m) on the coupling efficiency in plasma conditions relevant to compression and shock ignition (SI) schemes in different intensity regimes. A difficult issue was to produce interaction conditions that are equivalent for the two wavelengths. This was obtained by using plasma preformed from a solid target with a plasma-preforming beam at the same wavelength as the interaction beam. This produced an almost exponential density profile from vacuum to the critical density of the interaction beam in which all interaction mechanisms are taken into account. The growth and saturation of stimulated Brillouin scattering (SBS) have been measured at the two wavelengths, in backward as well as in near-backward directions. We have found that the SBS intensity threshold is similar to 1.5 times higher at 3 omega than at 2 omega in agreement with the I lambda dependence of the SBS gain. The SBS behaviour is very well reproduced by the linear calculations of the postprocessor PIRANAH, giving us confidence that we have a good control of the relevance of the experimental conditions for the study of the laser wavelength effect on laser-plasma coupling. When SBS reaches the saturation regime, same levels of reflectivity are measured at 2 and 3 omega. Numerical simulations were performed with the paraxial code HERA to study the contribution of the fluid mechanisms in the saturation of SBS, showing that pump depletion and interplay with filamentation are likely to be the most important processes in SBS saturation for these conditions. This scenario also applies to the SBS of shock ignition high-intensity beams. (C) 2012 American Institute of Physics. [doi: 10.1063/1.3677256]

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