2012
DOI: 10.1007/s11434-012-5243-7
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Study of stimulated Raman and Brillouin scattering in a finite interaction region under the convective instability condition

Abstract: We discuss stimulated Raman scattering (SRS) and stimulated Brillouin scattering (SBS) under the convective instability condition with a one-dimensional three-wave interaction (3WI) model. Using linear theory, we deduce the temporal growth rate, gain exponent, and reflectivity of the backward scattered wave in a finite interaction region. We find that the growth rate is not only determined by the laser intensity and plasma density and temperature, but also related to the spatial gain. The length of the interac… Show more

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Cited by 10 publications
(5 citation statements)
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“…Assuming the plasmas are local uniform, the standard linear one-dimensional SBS three-waves interaction equations in homogenous plasmas are [35][36][37] ( ∂ ∂t…”
Section: B Absolute and Convective Condition For Stimulated Brillouimentioning
confidence: 99%
See 1 more Smart Citation
“…Assuming the plasmas are local uniform, the standard linear one-dimensional SBS three-waves interaction equations in homogenous plasmas are [35][36][37] ( ∂ ∂t…”
Section: B Absolute and Convective Condition For Stimulated Brillouimentioning
confidence: 99%
“…Assuming that the ions average mass and average charge number are mi and Zi . Following Hao et al [36,38], one can obtain the usual SBS threshold γ thB = √ ν A ν s and the threshold of absolute SBS instability is…”
Section: B Absolute and Convective Condition For Stimulated Brillouin...mentioning
confidence: 99%
“…The SBS process where the incident light couples to IAW and a backward-scattered electromagnetic wave, can be described by the following system of coupled envelope equations [39][40][41], relevant to an inhomogeneous flowing plasma: The slowly varying complex envelopes A 0 , A 1 and dn e describe the incident light vector potential, the Brillouin reflected light vector potential and the IAW amplitude, respectively. The group velocities of the waves are given by where g LDs is the contribution to the linear Landau damping of IAW, w = q Ek m bs s s is the bounce frequency and n ds is the effective diffusion rate of the trapped particle for species s. Although, comparing with the linear Landau damping of IAW, the collisional damping of IAW is very small for SBS in high temperature plasmas [44][45][46][47][48][49], it is well-known that the Landau damping can be significantly reduced by the modification of the distribution near the wave's phase velocity due to particle trapping [29,30].…”
Section: The Three Coupled-mode Equations For Sbsmentioning
confidence: 99%
“…From the three-wave equations [29][30][31], the theoretical growth rate of SRS scattered light in homogeneous plasmas is [1,32]…”
Section: Theoretical Analysismentioning
confidence: 99%