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Kinetic simulations of stimulated Raman backscattering and related processes for the shock-ignition approach to inertial confinement fusion

机译:激振方法惯性约束聚变的受激拉曼反向散射动力学模拟及相关过程

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摘要

A detailed description of stimulated Raman backscattering and related processes for the purpose of inertial confinement fusion requires multi-dimensional kinetic simulations of a full speckle in a high-temperature, large-scale, inhomogeneous plasma. In particular for the shock-ignition scheme operating at high laser intensities, kinetic aspects are predominant. High- (I λ_o~2 ~ 5 × 10~(15) W μm ~2/cm~2) as well as low-intensity (I λ _o~2 ~ 10~(15) W μm~2/cm ~2) cases show the predominance of collisionless, collective processes for the interaction. While the two-plasmon decay instability and the cavitation scenario are hardly affected by intensity variation, inflationary Raman backscattering proves to be very sensitive. Brillouin backscattering evolves on longer time scales and dominates the reflectivities, although it is sensitive to the intensity. Filamentation and self-focusing do occur for all cases but on time scales too long to affect Raman backscattering.
机译:出于惯性约束聚变的目的,对受激拉曼反向散射和相关过程的详细描述需要在高温,大规模,非均质等离子体中对全散斑进行多维动力学模拟。特别是对于在高激光强度下运行的冲击点火方案,动力学方面是主要的。高强度(Iλ_o〜2〜5×10〜(15)Wμm〜2 / cm〜2)和低强度强度(Iλ_o〜2〜10〜(15)Wμm〜2 / cm〜2 )案例显示了无冲突的,集体的交互过程占主导地位。虽然两等离子体激元的衰变不稳定性和空化情况几乎不受强度变化的影响,但膨胀拉曼背向散射被证明是非常敏感的。布里渊后向散射在较长的时间尺度上演化并控制反射率,尽管它对强度敏感。在所有情况下都会发生细丝化和自聚焦,但是时间尺度太长而不会影响拉曼反向散射。

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