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- W2003248882 abstract "Laser radiation propagating in a laser-produced plasma, in the presence of a self-generated magnetic field ${mathit{B}}_{mathit{S}}$ can decay into an electron Bernstein wave and a sideband Langmuir wave. Near the critical density, the laser may be linearly mode converted into a Langmuir wave, which may parametrically excite an electron Bernstein wave and a Langmuir wave. Inhomogeneity in the ${mathit{B}}_{mathit{S}}$ field determines the convective threshold for resonant and quasimode decay processes. In a plasma with electron temperature ${mathit{T}}_{mathit{e}}$ensuremath{sim}0.5 keV and a ${mathit{B}}_{mathit{S}}$ field scale length of ensuremath{sim}100 ensuremath{mu}m the power threshold at a 1-ensuremath{mu}m wavelength turns out to be ${10}^{15}$ W/${mathrm{cm}}^{2}$. Above the threshold the growth rate is of the order of 3ifmmodetimeselsetexttimesfi{}${10}^{11}$ ${mathrm{s}}^{mathrm{ensuremath{-}}1}$ for a resonant decay and ${10}^{11}$ ${mathrm{s}}^{mathrm{ensuremath{-}}1}$ for a nonresonant quasimode decay. textcopyright{} 1996 The American Physical Society." @default.
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- W2003248882 date "1996-03-01" @default.
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- W2003248882 title "Laser–Bernstein-mode coupling in a laser-produced plasma" @default.
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- W2003248882 doi "https://doi.org/10.1103/physreve.53.2735" @default.
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