1984
DOI: 10.1063/1.864801
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Stimulated Raman scattering, two-plasmon decay, and hot electron generation from underdense plasmas at 0.35 μm

Abstract: Experimental studies of stimulated Raman back and side scattering, two-plasmon decay, and the generation of high-energy electrons in 0.35 μm laser plasma interaction are presented. To isolate the various phenomena occurring at different densities, we have attempted to control the maximum plasma density by varying the thickness of the foil targets. The scattered light frequency is used as a diagnostic to measure the peak plasma density. Time integrated and time resolved scattered spectra for variable plasma den… Show more

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Cited by 113 publications
(19 citation statements)
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“…1,2 The main impact of these electrons in laserfusion experiments is the possible preheat of the fuel that can reduce the effectiveness of the implosion. We study the preheat due to these electrons by measuring the K␣ line emission from high-Z layers in a planar-target geometry on the OMEGA 3 laser system.…”
Section: Introductionmentioning
confidence: 99%
“…1,2 The main impact of these electrons in laserfusion experiments is the possible preheat of the fuel that can reduce the effectiveness of the implosion. We study the preheat due to these electrons by measuring the K␣ line emission from high-Z layers in a planar-target geometry on the OMEGA 3 laser system.…”
Section: Introductionmentioning
confidence: 99%
“…Previous experiments have observed SQSR backscatter 3 -6 or have observed SQSR sidescatter that was orders of magnitude less efficient. 7 Other experiments, using l-/xm irradiation, either did not measure the angular distribution 8 or did not determine the scattering mechanism. 9 Second, the total SQSR yield (up to several percent) is at least three orders of magnitude larger than has been reported from previous experiments using solid targets.…”
mentioning
confidence: 99%
“…Electrons can be accelerated to high energies by the two-plasmon decay (TPD) instability [7] in which the incident electromagnetic wave decays into two electron plasma waves [8][9][10]. The instability grows rapidly through the resonant coupling of the electric field of the incident laser beam and the longitudinal electrostatic field of the two electron plasma waves.…”
mentioning
confidence: 99%