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Emission of submm-radiation by strong turbulent plasma at two-stream instability of high current REB

机译:强流湍流等离子体在大电流REB的两流不稳定性下的亚毫米辐射发射

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One of possible ways to generate submillimeter wave and THz radiation is to use transformation of plasma waves into electromagnetic radiation at strong Langmuir turbulence [1]. We had already described some implementation of such method at the GOL-3 experiments [2–4], wherein the mechanism of plasma heating was recognized as the excitation of strong Langmuir turbulence (LT) via a two-stream instability induced by the propagating high current beam. The detailed theoretical consideration of LT-induced electromagnetic emission from turbulent plasmas distinguishes two main processes responsible for electromagnetic radiation emission during the beam-plasma interaction at GOL-3. First, plasmon scattering on plasma density fluctuations yields electromagnetic emission at the plasma frequency ωp (“ωp-process”). Second, plasmon-plasmon merging results in production of photons in the vicinity of the double plasma frequency 2ωp (“2ωp-process”). For plasma densities of 1014–1015 cm−3, corresponding output radiation frequencies are located in the range from mm to sub-mm waves, ωP/2π ≌ 90–283 GHz, 2ωP/2π ≌ 180–566 GHz.
机译:产生亚毫米波和太赫兹辐射的一种可能方法是在强朗缪尔湍流下利用等离子波转换为电磁辐射[1]。我们已经在GOL-3实验中描述了这种方法的一些实现方法[2-4],其中等离子加热的机制被认为是由于高能传播引起的两股流不稳定性而激发的强朗缪尔湍流(LT)。当前光束。湍流等离子体对LT引起的电磁辐射的详细理论考虑,区分了在GOL-3的束流-等离子体相互作用过程中负责电磁辐射发射的两个主要过程。首先,等离子体密度波动引起的等离激元散射会产生等离子体频率ω p 的电磁辐射(“ω p 过程”)。其次,等离激元-等离激元合并会在双倍等离子体频率2ω p 附近产生光子(“2ω p 过程”)。对于10 14 –10 15 cm -3 的等离子体密度,相应的输出辐射频率位于毫米波到亚毫米波的范围内,ω P /2π≌90–283 GHz,2ω P /2π≌180–566 GHz。

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