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Generation of High-Power Sub-THz Waves in Magnetized Turbulent Electron Beam Plasmas
Sub-THz radiation can be generated by conversion of plasma waves into electromagnetic (EM) radiation in a plasma with strong Langmuir (LT) turbulence produced via a two-stream instability of a high current relativistic electron beam (REB). Nonlinear plasmon-plasmon merging results in the generation...
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Published in: | Journal of infrared, millimeter and terahertz waves millimeter and terahertz waves, 2014, Vol.35 (1), p.81-90 |
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creator | Thumm, M. K. A. Arzhannikov, A. V. Astrelin, V. T. Burdakov, A. V. Ivanov, I. A. Kalinin, P. V. Kandaurov, I. V. Kurkuchekov, V. V. Kuznetsov, S. A. Makarov, M. A. Mekler, K. I. Polosatkin, S. V. Popov, S. A. Postupaev, V. V. Rovenskikh, A. F. Sinitsky, S. L. Sklyarov, V. F. Stepanov, V. D. Trunev, Yu. A. Timofeev, I. V. Vyacheslavov, L. N. |
description | Sub-THz radiation can be generated by conversion of plasma waves into electromagnetic (EM) radiation in a plasma with strong Langmuir (LT) turbulence produced via a two-stream instability of a high current relativistic electron beam (REB). Nonlinear plasmon-plasmon merging results in the generation of photons nearby the 2
nd
harmonic of the plasma frequency 2
ω
p
(“2
ω
p
-process”). For plasma densities of 10
14
− 10
15
cm
−3
, these frequencies are in the range of sub-THz waves at 370–570 GHz. The specific power density of sub-THz-wave emission from plasmas in the multi-mirror magnetic trap GOL-3 (at BINP) during injection of a 10-μs-REB with a current density of about 1 kA/cm
2
at plasma densities
n
e
≈ 5∙10
14
cm
−3
, electron temperatures
T
e
≈ 1.5 keV and magnetic induction
B
≈ 4 T was measured to be approx. 1 kW/cm
3
in the frequency band around 300 GHz. In the case of a weakly relativistic 100-μs-electron beam (90 keV) with 250 A/cm
2
the corresponding results are 700 W/cm
3
around 90 GHz with an efficiency of 1–2 % at
n
e
≈ 3∙10
13
cm
−3
(total power ≈ 30 kW). Theoretical investigations show that at a density of
n
e
≈ 3∙10
15
cm
−3
and a turbulence level of 5 % the generated sub-THz power can reach ≈ 1 MW/cm
3
. |
doi_str_mv | 10.1007/s10762-013-9969-3 |
format | article |
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nd
harmonic of the plasma frequency 2
ω
p
(“2
ω
p
-process”). For plasma densities of 10
14
− 10
15
cm
−3
, these frequencies are in the range of sub-THz waves at 370–570 GHz. The specific power density of sub-THz-wave emission from plasmas in the multi-mirror magnetic trap GOL-3 (at BINP) during injection of a 10-μs-REB with a current density of about 1 kA/cm
2
at plasma densities
n
e
≈ 5∙10
14
cm
−3
, electron temperatures
T
e
≈ 1.5 keV and magnetic induction
B
≈ 4 T was measured to be approx. 1 kW/cm
3
in the frequency band around 300 GHz. In the case of a weakly relativistic 100-μs-electron beam (90 keV) with 250 A/cm
2
the corresponding results are 700 W/cm
3
around 90 GHz with an efficiency of 1–2 % at
n
e
≈ 3∙10
13
cm
−3
(total power ≈ 30 kW). Theoretical investigations show that at a density of
n
e
≈ 3∙10
15
cm
−3
and a turbulence level of 5 % the generated sub-THz power can reach ≈ 1 MW/cm
3
.</description><identifier>ISSN: 1866-6892</identifier><identifier>EISSN: 1866-6906</identifier><identifier>DOI: 10.1007/s10762-013-9969-3</identifier><language>eng</language><publisher>Boston: Springer US</publisher><subject>Classical Electrodynamics ; Current density ; Density ; Electrical Engineering ; Electronics and Microelectronics ; Engineering ; Fluid dynamics ; Fluid flow ; Instrumentation ; Plasma density ; Plasmas ; Turbulence ; Turbulent flow</subject><ispartof>Journal of infrared, millimeter and terahertz waves, 2014, Vol.35 (1), p.81-90</ispartof><rights>Springer Science+Business Media New York 2013</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c251t-4fd79ad6adaa20743ee65f3e43ae4f61d92643856819b0167cc48ee5f34689093</citedby><cites>FETCH-LOGICAL-c251t-4fd79ad6adaa20743ee65f3e43ae4f61d92643856819b0167cc48ee5f34689093</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Thumm, M. K. A.</creatorcontrib><creatorcontrib>Arzhannikov, A. V.</creatorcontrib><creatorcontrib>Astrelin, V. T.</creatorcontrib><creatorcontrib>Burdakov, A. V.</creatorcontrib><creatorcontrib>Ivanov, I. A.</creatorcontrib><creatorcontrib>Kalinin, P. V.</creatorcontrib><creatorcontrib>Kandaurov, I. V.</creatorcontrib><creatorcontrib>Kurkuchekov, V. V.</creatorcontrib><creatorcontrib>Kuznetsov, S. A.</creatorcontrib><creatorcontrib>Makarov, M. A.</creatorcontrib><creatorcontrib>Mekler, K. I.</creatorcontrib><creatorcontrib>Polosatkin, S. V.</creatorcontrib><creatorcontrib>Popov, S. A.</creatorcontrib><creatorcontrib>Postupaev, V. V.</creatorcontrib><creatorcontrib>Rovenskikh, A. F.</creatorcontrib><creatorcontrib>Sinitsky, S. L.</creatorcontrib><creatorcontrib>Sklyarov, V. F.</creatorcontrib><creatorcontrib>Stepanov, V. D.</creatorcontrib><creatorcontrib>Trunev, Yu. A.</creatorcontrib><creatorcontrib>Timofeev, I. V.</creatorcontrib><creatorcontrib>Vyacheslavov, L. N.</creatorcontrib><title>Generation of High-Power Sub-THz Waves in Magnetized Turbulent Electron Beam Plasmas</title><title>Journal of infrared, millimeter and terahertz waves</title><addtitle>J Infrared Milli Terahz Waves</addtitle><description>Sub-THz radiation can be generated by conversion of plasma waves into electromagnetic (EM) radiation in a plasma with strong Langmuir (LT) turbulence produced via a two-stream instability of a high current relativistic electron beam (REB). Nonlinear plasmon-plasmon merging results in the generation of photons nearby the 2
nd
harmonic of the plasma frequency 2
ω
p
(“2
ω
p
-process”). For plasma densities of 10
14
− 10
15
cm
−3
, these frequencies are in the range of sub-THz waves at 370–570 GHz. The specific power density of sub-THz-wave emission from plasmas in the multi-mirror magnetic trap GOL-3 (at BINP) during injection of a 10-μs-REB with a current density of about 1 kA/cm
2
at plasma densities
n
e
≈ 5∙10
14
cm
−3
, electron temperatures
T
e
≈ 1.5 keV and magnetic induction
B
≈ 4 T was measured to be approx. 1 kW/cm
3
in the frequency band around 300 GHz. In the case of a weakly relativistic 100-μs-electron beam (90 keV) with 250 A/cm
2
the corresponding results are 700 W/cm
3
around 90 GHz with an efficiency of 1–2 % at
n
e
≈ 3∙10
13
cm
−3
(total power ≈ 30 kW). Theoretical investigations show that at a density of
n
e
≈ 3∙10
15
cm
−3
and a turbulence level of 5 % the generated sub-THz power can reach ≈ 1 MW/cm
3
.</description><subject>Classical Electrodynamics</subject><subject>Current density</subject><subject>Density</subject><subject>Electrical Engineering</subject><subject>Electronics and Microelectronics</subject><subject>Engineering</subject><subject>Fluid dynamics</subject><subject>Fluid flow</subject><subject>Instrumentation</subject><subject>Plasma density</subject><subject>Plasmas</subject><subject>Turbulence</subject><subject>Turbulent flow</subject><issn>1866-6892</issn><issn>1866-6906</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNp9kD1PwzAQQC0EEqXwA9g8shj8FSceoYIWqYhKBDFabnIpqRK72AmI_npSBVamu-G9k-4hdMnoNaM0vYmMpooTygTRWmkijtCEZUoRpak6_tszzU_RWYxbSpWUWk1QPgcHwXa1d9hXeFFv3snKf0HAL_2a5Is9frOfEHHt8JPdOOjqPZQ478O6b8B1-L6BoguDfAe2xavGxtbGc3RS2SbCxe-coteH-3y2IMvn-ePsdkkKnrCOyKpMtS2VLa3lNJUCQCWVACksyEqxUnMlRZaojOk1ZSotCpkBDIgcPqFaTNHVeHcX_EcPsTNtHQtoGuvA99GwhFMtMyEPKBvRIvgYA1RmF-rWhm_DqDkUNGNBMxQ0h4JGDA4fnTiwbgPBbH0f3PDRP9IPgGdy3A</recordid><startdate>2014</startdate><enddate>2014</enddate><creator>Thumm, M. K. A.</creator><creator>Arzhannikov, A. V.</creator><creator>Astrelin, V. T.</creator><creator>Burdakov, A. V.</creator><creator>Ivanov, I. A.</creator><creator>Kalinin, P. V.</creator><creator>Kandaurov, I. V.</creator><creator>Kurkuchekov, V. V.</creator><creator>Kuznetsov, S. A.</creator><creator>Makarov, M. A.</creator><creator>Mekler, K. I.</creator><creator>Polosatkin, S. V.</creator><creator>Popov, S. A.</creator><creator>Postupaev, V. V.</creator><creator>Rovenskikh, A. F.</creator><creator>Sinitsky, S. L.</creator><creator>Sklyarov, V. F.</creator><creator>Stepanov, V. D.</creator><creator>Trunev, Yu. A.</creator><creator>Timofeev, I. V.</creator><creator>Vyacheslavov, L. N.</creator><general>Springer US</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>FR3</scope><scope>KR7</scope><scope>L7M</scope></search><sort><creationdate>2014</creationdate><title>Generation of High-Power Sub-THz Waves in Magnetized Turbulent Electron Beam Plasmas</title><author>Thumm, M. K. A. ; Arzhannikov, A. V. ; Astrelin, V. T. ; Burdakov, A. V. ; Ivanov, I. A. ; Kalinin, P. V. ; Kandaurov, I. V. ; Kurkuchekov, V. V. ; Kuznetsov, S. A. ; Makarov, M. A. ; Mekler, K. I. ; Polosatkin, S. V. ; Popov, S. A. ; Postupaev, V. V. ; Rovenskikh, A. F. ; Sinitsky, S. L. ; Sklyarov, V. F. ; Stepanov, V. D. ; Trunev, Yu. A. ; Timofeev, I. V. ; Vyacheslavov, L. N.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c251t-4fd79ad6adaa20743ee65f3e43ae4f61d92643856819b0167cc48ee5f34689093</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Classical Electrodynamics</topic><topic>Current density</topic><topic>Density</topic><topic>Electrical Engineering</topic><topic>Electronics and Microelectronics</topic><topic>Engineering</topic><topic>Fluid dynamics</topic><topic>Fluid flow</topic><topic>Instrumentation</topic><topic>Plasma density</topic><topic>Plasmas</topic><topic>Turbulence</topic><topic>Turbulent flow</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Thumm, M. K. A.</creatorcontrib><creatorcontrib>Arzhannikov, A. V.</creatorcontrib><creatorcontrib>Astrelin, V. T.</creatorcontrib><creatorcontrib>Burdakov, A. V.</creatorcontrib><creatorcontrib>Ivanov, I. A.</creatorcontrib><creatorcontrib>Kalinin, P. V.</creatorcontrib><creatorcontrib>Kandaurov, I. V.</creatorcontrib><creatorcontrib>Kurkuchekov, V. V.</creatorcontrib><creatorcontrib>Kuznetsov, S. A.</creatorcontrib><creatorcontrib>Makarov, M. A.</creatorcontrib><creatorcontrib>Mekler, K. I.</creatorcontrib><creatorcontrib>Polosatkin, S. V.</creatorcontrib><creatorcontrib>Popov, S. A.</creatorcontrib><creatorcontrib>Postupaev, V. V.</creatorcontrib><creatorcontrib>Rovenskikh, A. F.</creatorcontrib><creatorcontrib>Sinitsky, S. L.</creatorcontrib><creatorcontrib>Sklyarov, V. F.</creatorcontrib><creatorcontrib>Stepanov, V. D.</creatorcontrib><creatorcontrib>Trunev, Yu. A.</creatorcontrib><creatorcontrib>Timofeev, I. V.</creatorcontrib><creatorcontrib>Vyacheslavov, L. N.</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of infrared, millimeter and terahertz waves</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Thumm, M. K. A.</au><au>Arzhannikov, A. V.</au><au>Astrelin, V. T.</au><au>Burdakov, A. V.</au><au>Ivanov, I. A.</au><au>Kalinin, P. V.</au><au>Kandaurov, I. V.</au><au>Kurkuchekov, V. V.</au><au>Kuznetsov, S. A.</au><au>Makarov, M. A.</au><au>Mekler, K. I.</au><au>Polosatkin, S. V.</au><au>Popov, S. A.</au><au>Postupaev, V. V.</au><au>Rovenskikh, A. F.</au><au>Sinitsky, S. L.</au><au>Sklyarov, V. F.</au><au>Stepanov, V. D.</au><au>Trunev, Yu. A.</au><au>Timofeev, I. V.</au><au>Vyacheslavov, L. N.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Generation of High-Power Sub-THz Waves in Magnetized Turbulent Electron Beam Plasmas</atitle><jtitle>Journal of infrared, millimeter and terahertz waves</jtitle><stitle>J Infrared Milli Terahz Waves</stitle><date>2014</date><risdate>2014</risdate><volume>35</volume><issue>1</issue><spage>81</spage><epage>90</epage><pages>81-90</pages><issn>1866-6892</issn><eissn>1866-6906</eissn><abstract>Sub-THz radiation can be generated by conversion of plasma waves into electromagnetic (EM) radiation in a plasma with strong Langmuir (LT) turbulence produced via a two-stream instability of a high current relativistic electron beam (REB). Nonlinear plasmon-plasmon merging results in the generation of photons nearby the 2
nd
harmonic of the plasma frequency 2
ω
p
(“2
ω
p
-process”). For plasma densities of 10
14
− 10
15
cm
−3
, these frequencies are in the range of sub-THz waves at 370–570 GHz. The specific power density of sub-THz-wave emission from plasmas in the multi-mirror magnetic trap GOL-3 (at BINP) during injection of a 10-μs-REB with a current density of about 1 kA/cm
2
at plasma densities
n
e
≈ 5∙10
14
cm
−3
, electron temperatures
T
e
≈ 1.5 keV and magnetic induction
B
≈ 4 T was measured to be approx. 1 kW/cm
3
in the frequency band around 300 GHz. In the case of a weakly relativistic 100-μs-electron beam (90 keV) with 250 A/cm
2
the corresponding results are 700 W/cm
3
around 90 GHz with an efficiency of 1–2 % at
n
e
≈ 3∙10
13
cm
−3
(total power ≈ 30 kW). Theoretical investigations show that at a density of
n
e
≈ 3∙10
15
cm
−3
and a turbulence level of 5 % the generated sub-THz power can reach ≈ 1 MW/cm
3
.</abstract><cop>Boston</cop><pub>Springer US</pub><doi>10.1007/s10762-013-9969-3</doi><tpages>10</tpages></addata></record> |
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subjects | Classical Electrodynamics Current density Density Electrical Engineering Electronics and Microelectronics Engineering Fluid dynamics Fluid flow Instrumentation Plasma density Plasmas Turbulence Turbulent flow |
title | Generation of High-Power Sub-THz Waves in Magnetized Turbulent Electron Beam Plasmas |
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