强湍流等离子体在大电流REB双流不稳定性下的亚毫米辐射发射

A. Arzhannikov, A. Burdakov, P. V. Kalinin, S. Kuznetsov, M. Makarov, K. Mekler, A. Popov, V. Postupaev, A. Rovenskikh, S. Sinitsky, V. Sklyarov, V. Stepanov, Y. Sulyaev, M. Thumm, L. Vyacheslavov
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引用次数: 1

摘要

产生亚毫米波和太赫兹辐射的一种可能方法是在强Langmuir湍流下将等离子体波转化为电磁辐射[1]。我们已经在go -3实验中描述了这种方法的一些实现[2-4],其中等离子体加热的机制被认为是通过传播的大电流光束引起的两流不稳定性来激发强朗缪尔湍流(LT)。对湍流等离子体的热致电磁辐射进行了详细的理论研究,区分了在go3的束流-等离子体相互作用中产生电磁辐射的两个主要过程。首先,等离子体密度波动引起的等离子体激元散射产生的电磁发射频率为ωp(“ωp过程”)。其次,等离子体-等离子体合并导致在双等离子体频率2ωp附近产生光子(“2ωp过程”)。等离子体密度为1014 ~ 1015 cm−3时,对应的输出辐射频率在mm ~亚mm波范围内,ωP/2π≌90 ~ 283 GHz, 2ωP/2π≌180 ~ 566 GHz。
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Emission of submm-radiation by strong turbulent plasma at two-stream instability of high current REB
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.
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