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":"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","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":"{\"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}","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}
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.