Nikolić Lj, Skorić M M, Ishiguro S, Sato T
The Graduate University for Advanced Studies, National Institute for Fusion Science, 322-6 Oroshi-cho, Toki-shi 509-5292, Japan.
Phys Rev E Stat Nonlin Soft Matter Phys. 2002 Sep;66(3 Pt 2B):036404. doi: 10.1103/PhysRevE.66.036404. Epub 2002 Sep 20.
Intense laser-plasma interaction can be a source of various electronic instabilities. Recently, stimulated backscattering from a trapped electron-acoustic wave (SEAS) [Montgomery et al., Phys. Rev. Lett. 87, 155001 (2001)] was proposed to reinterpret spectra previously attributed to stimulated Raman scattering (SRS) from unrealistically low densities. By particle simulations in a uniform plasma layer, which is overdense for ordinary SRS, strong reflection by SEAS at the electron plasma frequency is found. Transient SEAS reflectivity pulsations are followed by strong relativistic heating of electrons. Physical conditions are explained by three-wave parametric coupling between laser light, standing backscattered wave and slow electron-acoustic wave. Regions in which SEAS reflection can dominate over SRS are singled out.
强激光与等离子体相互作用可能是各种电子不稳定性的一个来源。最近,有人提出用从俘获电子声波产生的受激背向散射(SEAS)[蒙哥马利等人,《物理评论快报》87, 155001 (2001)] 来重新解释以前归因于来自不切实际的低密度的受激拉曼散射(SRS)的光谱。通过在均匀等离子体层中的粒子模拟(对于普通SRS来说该等离子体层是过密的),发现在电子等离子体频率处有SEAS的强反射。SEAS反射率的瞬态脉动之后是电子的强烈相对论性加热。物理条件由激光、驻波背向散射波和慢电子声波之间的三波参数耦合来解释。确定了SEAS反射能够比SRS占主导的区域。