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
{"title":"Emission of submm-radiation by strong turbulent plasma at two-stream instability of high current REB","authors":"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","doi":"10.1109/IRMMW-THZ.2011.6105246","DOIUrl":null,"url":null,"abstract":"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 ω<inf>p</inf> (“ω<inf>p</inf>-process”). Second, plasmon-plasmon merging results in production of photons in the vicinity of the double plasma frequency 2ω<inf>p</inf> (“2ω<inf>p</inf>-process”). For plasma densities of 10<sup>14</sup>–10<sup>15</sup> cm<sup>−3</sup>, corresponding output radiation frequencies are located in the range from mm to sub-mm waves, ω<inf>P</inf>/2π ≌ 90–283 GHz, 2ω<inf>P</inf>/2π ≌ 180–566 GHz.","PeriodicalId":6353,"journal":{"name":"2011 International Conference on Infrared, Millimeter, and Terahertz Waves","volume":"36 1","pages":"1-2"},"PeriodicalIF":0.0000,"publicationDate":"2011-12-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2011 International Conference on Infrared, Millimeter, and Terahertz Waves","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IRMMW-THZ.2011.6105246","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
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.