3-d reconfiguration of electromagnetic field in multiwave cerenkov generator
Summary form only given. To date, the record power in X-band and millimeter-wave band is realized relativistic multiwave devices. The best result (15 GW in X-band) was obtained in the multiwave Cerenkov generator (MWCG). Design features of MWCG are the following: a) 3-D oversized electrodynamics sys...
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creator | Cherepenin, Vladimir A. Kornienko, Vladimir N. |
description | Summary form only given. To date, the record power in X-band and millimeter-wave band is realized relativistic multiwave devices. The best result (15 GW in X-band) was obtained in the multiwave Cerenkov generator (MWCG). Design features of MWCG are the following: a) 3-D oversized electrodynamics system: b) the generation frequency is determined by the interaction between electron beam and electromagnetic field at the frequency close to the cutoff of periodical system; c) focusing static magnetic field plays important role in the interaction process. The possibility to use PIC-codes for analysis of multiwave devices has appeared just recently. In this paper the results of computer simulations of two-section MWCG are presented. Parameters of electron beam and electrodynamics system correspond to the experimental device. Spatial distribution of the RF field in the MWCG was tracked from generation start up to the maximum of beam current. The influence of the operating mode in the first section on the evolution of radiation spectrum was studied. Operating mode depends on the reflection of electromagnetic wave from the cathode. It was showed that two modes can be realized mainly. Each of them has specific spatial distribution of electromagnetic field. In the first mode, the stationary radiation lasts for 50-60 ns. It's frequency is about 11-12 GHz. After this time mode hopping takes place. In the second mode, the spectrum of radiation and power remain constant during 100 ns. |
doi_str_mv | 10.1109/PPPS.2007.4346334 |
format | Conference Proceeding |
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To date, the record power in X-band and millimeter-wave band is realized relativistic multiwave devices. The best result (15 GW in X-band) was obtained in the multiwave Cerenkov generator (MWCG). Design features of MWCG are the following: a) 3-D oversized electrodynamics system: b) the generation frequency is determined by the interaction between electron beam and electromagnetic field at the frequency close to the cutoff of periodical system; c) focusing static magnetic field plays important role in the interaction process. The possibility to use PIC-codes for analysis of multiwave devices has appeared just recently. In this paper the results of computer simulations of two-section MWCG are presented. Parameters of electron beam and electrodynamics system correspond to the experimental device. Spatial distribution of the RF field in the MWCG was tracked from generation start up to the maximum of beam current. The influence of the operating mode in the first section on the evolution of radiation spectrum was studied. Operating mode depends on the reflection of electromagnetic wave from the cathode. It was showed that two modes can be realized mainly. Each of them has specific spatial distribution of electromagnetic field. In the first mode, the stationary radiation lasts for 50-60 ns. It's frequency is about 11-12 GHz. After this time mode hopping takes place. In the second mode, the spectrum of radiation and power remain constant during 100 ns.</description><identifier>ISSN: 0730-9244</identifier><identifier>ISBN: 9781424409150</identifier><identifier>ISBN: 1424409152</identifier><identifier>EISSN: 2576-7208</identifier><identifier>DOI: 10.1109/PPPS.2007.4346334</identifier><identifier>LCCN: 81-644315</identifier><language>eng</language><publisher>IEEE</publisher><subject>Computer simulation ; Cutoff frequency ; Electrodynamics ; Electromagnetic fields ; Electromagnetic reflection ; Electron beams ; Magnetic analysis ; Magnetic fields ; Optical reflection ; Radio frequency</subject><ispartof>2007 IEEE 34th International Conference on Plasma Science (ICOPS), 2007, p.1028-1028</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/4346334$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>309,310,776,780,785,786,2051,27904,54898</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/4346334$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Cherepenin, Vladimir A.</creatorcontrib><creatorcontrib>Kornienko, Vladimir N.</creatorcontrib><title>3-d reconfiguration of electromagnetic field in multiwave cerenkov generator</title><title>2007 IEEE 34th International Conference on Plasma Science (ICOPS)</title><addtitle>PLASMA</addtitle><description>Summary form only given. To date, the record power in X-band and millimeter-wave band is realized relativistic multiwave devices. The best result (15 GW in X-band) was obtained in the multiwave Cerenkov generator (MWCG). Design features of MWCG are the following: a) 3-D oversized electrodynamics system: b) the generation frequency is determined by the interaction between electron beam and electromagnetic field at the frequency close to the cutoff of periodical system; c) focusing static magnetic field plays important role in the interaction process. The possibility to use PIC-codes for analysis of multiwave devices has appeared just recently. In this paper the results of computer simulations of two-section MWCG are presented. Parameters of electron beam and electrodynamics system correspond to the experimental device. Spatial distribution of the RF field in the MWCG was tracked from generation start up to the maximum of beam current. The influence of the operating mode in the first section on the evolution of radiation spectrum was studied. Operating mode depends on the reflection of electromagnetic wave from the cathode. It was showed that two modes can be realized mainly. Each of them has specific spatial distribution of electromagnetic field. In the first mode, the stationary radiation lasts for 50-60 ns. It's frequency is about 11-12 GHz. After this time mode hopping takes place. In the second mode, the spectrum of radiation and power remain constant during 100 ns.</description><subject>Computer simulation</subject><subject>Cutoff frequency</subject><subject>Electrodynamics</subject><subject>Electromagnetic fields</subject><subject>Electromagnetic reflection</subject><subject>Electron beams</subject><subject>Magnetic analysis</subject><subject>Magnetic fields</subject><subject>Optical reflection</subject><subject>Radio frequency</subject><issn>0730-9244</issn><issn>2576-7208</issn><isbn>9781424409150</isbn><isbn>1424409152</isbn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2007</creationdate><recordtype>conference_proceeding</recordtype><sourceid>6IE</sourceid><sourceid>RIE</sourceid><recordid>eNp9jsFqwzAQRJe0gZrWHxB60Q_IXVlryzqXlh56MKT3IJy1UWNLQXZS-vf1IefOZeANDwZgp7BQCu1L27b7okQ0BWmqtaYNZGVlamlKbO4gt6ZRVBKhVRXeQ4ZGo7Qr2ELWKFkTaVU9QD7P37iGKlJkM_jU8igSdzH0frgkt_gYROwFj9wtKU5uCLz4TvSex6PwQUyXcfE_7sqi48ThFK9i4MCrGdMTbHs3zpzf-hGe39--Xj-kZ-bDOfnJpd_D7b_-f_0DxGFEDg</recordid><startdate>200706</startdate><enddate>200706</enddate><creator>Cherepenin, Vladimir A.</creator><creator>Kornienko, Vladimir N.</creator><general>IEEE</general><scope>6IE</scope><scope>6IH</scope><scope>CBEJK</scope><scope>RIE</scope><scope>RIO</scope></search><sort><creationdate>200706</creationdate><title>3-d reconfiguration of electromagnetic field in multiwave cerenkov generator</title><author>Cherepenin, Vladimir A. ; Kornienko, Vladimir N.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-ieee_primary_43463343</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2007</creationdate><topic>Computer simulation</topic><topic>Cutoff frequency</topic><topic>Electrodynamics</topic><topic>Electromagnetic fields</topic><topic>Electromagnetic reflection</topic><topic>Electron beams</topic><topic>Magnetic analysis</topic><topic>Magnetic fields</topic><topic>Optical reflection</topic><topic>Radio frequency</topic><toplevel>online_resources</toplevel><creatorcontrib>Cherepenin, Vladimir A.</creatorcontrib><creatorcontrib>Kornienko, Vladimir N.</creatorcontrib><collection>IEEE Electronic Library (IEL) Conference Proceedings</collection><collection>IEEE Proceedings Order Plan (POP) 1998-present by volume</collection><collection>IEEE Xplore All Conference Proceedings</collection><collection>IEEE Electronic Library (IEL)</collection><collection>IEEE Proceedings Order Plans (POP) 1998-present</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Cherepenin, Vladimir A.</au><au>Kornienko, Vladimir N.</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>3-d reconfiguration of electromagnetic field in multiwave cerenkov generator</atitle><btitle>2007 IEEE 34th International Conference on Plasma Science (ICOPS)</btitle><stitle>PLASMA</stitle><date>2007-06</date><risdate>2007</risdate><spage>1028</spage><epage>1028</epage><pages>1028-1028</pages><issn>0730-9244</issn><eissn>2576-7208</eissn><isbn>9781424409150</isbn><isbn>1424409152</isbn><abstract>Summary form only given. To date, the record power in X-band and millimeter-wave band is realized relativistic multiwave devices. The best result (15 GW in X-band) was obtained in the multiwave Cerenkov generator (MWCG). Design features of MWCG are the following: a) 3-D oversized electrodynamics system: b) the generation frequency is determined by the interaction between electron beam and electromagnetic field at the frequency close to the cutoff of periodical system; c) focusing static magnetic field plays important role in the interaction process. The possibility to use PIC-codes for analysis of multiwave devices has appeared just recently. In this paper the results of computer simulations of two-section MWCG are presented. Parameters of electron beam and electrodynamics system correspond to the experimental device. Spatial distribution of the RF field in the MWCG was tracked from generation start up to the maximum of beam current. The influence of the operating mode in the first section on the evolution of radiation spectrum was studied. Operating mode depends on the reflection of electromagnetic wave from the cathode. It was showed that two modes can be realized mainly. Each of them has specific spatial distribution of electromagnetic field. In the first mode, the stationary radiation lasts for 50-60 ns. It's frequency is about 11-12 GHz. After this time mode hopping takes place. In the second mode, the spectrum of radiation and power remain constant during 100 ns.</abstract><pub>IEEE</pub><doi>10.1109/PPPS.2007.4346334</doi></addata></record> |
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ispartof | 2007 IEEE 34th International Conference on Plasma Science (ICOPS), 2007, p.1028-1028 |
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language | eng |
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source | IEEE Electronic Library (IEL) Conference Proceedings |
subjects | Computer simulation Cutoff frequency Electrodynamics Electromagnetic fields Electromagnetic reflection Electron beams Magnetic analysis Magnetic fields Optical reflection Radio frequency |
title | 3-d reconfiguration of electromagnetic field in multiwave cerenkov generator |
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