Novosibirsk Free Electron Laser: Recent Achievements and Future Prospects
Free electron lasers (FELs) are unique sources of electromagnetic radiation with tunable wavelength. A high-power FEL has been created at the G. I.Budker Institute for Nuclear Physics. Its radiation frequency can be tuned over a wide range in the terahertz and infrared spectral ranges. As the source...
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creator | Shevchenko, O. A. Arbuzov, V. S. Vinokurov, N. A. Vobly, P. D. Volkov, V. N. Getmanov, Ya. V Davidyuk, I. V. Deychuly, O. I. Dementyev, E. N. Dovzhenko, B. A. Knyazev, B. A. Kolobanov, E. I. Kondakov, A. A. Kozak, V. R. Kozyrev, E. V. Kubarev, V. V. Kulipanov, G. N. Kuper, E. A. Kuptsov, I. V. Kurkin, G. Ya Krutikhin, S. A. Medvedev, L. E. Motygin, S. V. Ovchar, V. K. Osipov, V. N. Petrov, V. M. Pilan, A. M. Popik, V. M. Repkov, V. V. Salikova, T. V. Sedlyarov, I. K. Serednyakov, S. S. Skrinsky, A. N. Tararyshkin, S. V. Tribendis, A. G. Cheskidov, V. G. Chernov, K. N. Shcheglov, M. A. |
description | Free electron lasers (FELs) are unique sources of electromagnetic radiation with tunable wavelength. A high-power FEL has been created at the G. I.Budker Institute for Nuclear Physics. Its radiation frequency can be tuned over a wide range in the terahertz and infrared spectral ranges. As the source of electron bunches, this FEL uses a multi-turn energy-recovery linac, which has five straight sections. Three sections are used for three FELs which operate in different wavelength ranges (90–240 μm for the first, 37–80 μm for the second, and 5–20 μm for the third ones). The first and the second FELs were commissioned in 2003 and 2009, respectively. They are used for various applied and research problems now. The third FEL is installed on the last, forth accelerator loop, in which the electron energy is the maximum. It comprises three undulator sections and a 40 m optical cavity. The first lasing of this FEL was obtained in the summer of 2015. The radiation wavelength was 9 μm and the average power was about 100 W. The design power is 1 kW at a pulse repetition rate of 3.75 MHz. Radiation of the third FEL will be delivered to user stations from the protected hall in the near future. The third FEL commissioning results are presented and the current status of the first and second FELs as well as their future development prospects are described. |
doi_str_mv | 10.1007/s11141-017-9727-9 |
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A. ; Arbuzov, V. S. ; Vinokurov, N. A. ; Vobly, P. D. ; Volkov, V. N. ; Getmanov, Ya. V ; Davidyuk, I. V. ; Deychuly, O. I. ; Dementyev, E. N. ; Dovzhenko, B. A. ; Knyazev, B. A. ; Kolobanov, E. I. ; Kondakov, A. A. ; Kozak, V. R. ; Kozyrev, E. V. ; Kubarev, V. V. ; Kulipanov, G. N. ; Kuper, E. A. ; Kuptsov, I. V. ; Kurkin, G. Ya ; Krutikhin, S. A. ; Medvedev, L. E. ; Motygin, S. V. ; Ovchar, V. K. ; Osipov, V. N. ; Petrov, V. M. ; Pilan, A. M. ; Popik, V. M. ; Repkov, V. V. ; Salikova, T. V. ; Sedlyarov, I. K. ; Serednyakov, S. S. ; Skrinsky, A. N. ; Tararyshkin, S. V. ; Tribendis, A. G. ; Cheskidov, V. G. ; Chernov, K. N. ; Shcheglov, M. A.</creator><creatorcontrib>Shevchenko, O. A. ; Arbuzov, V. S. ; Vinokurov, N. A. ; Vobly, P. D. ; Volkov, V. N. ; Getmanov, Ya. V ; Davidyuk, I. V. ; Deychuly, O. I. ; Dementyev, E. N. ; Dovzhenko, B. A. ; Knyazev, B. A. ; Kolobanov, E. I. ; Kondakov, A. A. ; Kozak, V. R. ; Kozyrev, E. V. ; Kubarev, V. V. ; Kulipanov, G. N. ; Kuper, E. A. ; Kuptsov, I. V. ; Kurkin, G. Ya ; Krutikhin, S. A. ; Medvedev, L. E. ; Motygin, S. V. ; Ovchar, V. K. ; Osipov, V. N. ; Petrov, V. M. ; Pilan, A. M. ; Popik, V. M. ; Repkov, V. V. ; Salikova, T. V. ; Sedlyarov, I. K. ; Serednyakov, S. S. ; Skrinsky, A. N. ; Tararyshkin, S. V. ; Tribendis, A. G. ; Cheskidov, V. G. ; Chernov, K. N. ; Shcheglov, M. A.</creatorcontrib><description>Free electron lasers (FELs) are unique sources of electromagnetic radiation with tunable wavelength. A high-power FEL has been created at the G. I.Budker Institute for Nuclear Physics. Its radiation frequency can be tuned over a wide range in the terahertz and infrared spectral ranges. As the source of electron bunches, this FEL uses a multi-turn energy-recovery linac, which has five straight sections. Three sections are used for three FELs which operate in different wavelength ranges (90–240 μm for the first, 37–80 μm for the second, and 5–20 μm for the third ones). The first and the second FELs were commissioned in 2003 and 2009, respectively. They are used for various applied and research problems now. The third FEL is installed on the last, forth accelerator loop, in which the electron energy is the maximum. It comprises three undulator sections and a 40 m optical cavity. The first lasing of this FEL was obtained in the summer of 2015. The radiation wavelength was 9 μm and the average power was about 100 W. The design power is 1 kW at a pulse repetition rate of 3.75 MHz. Radiation of the third FEL will be delivered to user stations from the protected hall in the near future. The third FEL commissioning results are presented and the current status of the first and second FELs as well as their future development prospects are described.</description><identifier>ISSN: 0033-8443</identifier><identifier>EISSN: 1573-9120</identifier><identifier>DOI: 10.1007/s11141-017-9727-9</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Accelerators ; Astronomy ; Astrophysics and Astroparticles ; Electromagnetic radiation ; Electromagnetism ; Electrons ; Free electron lasers ; Hadrons ; Heavy Ions ; Infrared ; Lasers ; Lasing ; Mathematical and Computational Physics ; Nuclear Physics ; Nuclear power generation ; Observations and Techniques ; Optical Devices ; Optics ; Photonics ; Physics ; Physics and Astronomy ; Quantum Optics ; Spectra ; Stations ; Theoretical ; Wavelengths</subject><ispartof>Radiophysics and quantum electronics, 2017, Vol.59 (8-9), p.605-612</ispartof><rights>Springer Science+Business Media New York 2017</rights><rights>COPYRIGHT 2017 Springer</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c360t-ce0cbddef16fcd3f8af4a09eab734aaf1ffa191a1dfd68ed43776915f3b082833</citedby><cites>FETCH-LOGICAL-c360t-ce0cbddef16fcd3f8af4a09eab734aaf1ffa191a1dfd68ed43776915f3b082833</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11141-017-9727-9$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11141-017-9727-9$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27901,27902,41464,42533,51294</link.rule.ids></links><search><creatorcontrib>Shevchenko, O. A.</creatorcontrib><creatorcontrib>Arbuzov, V. S.</creatorcontrib><creatorcontrib>Vinokurov, N. A.</creatorcontrib><creatorcontrib>Vobly, P. D.</creatorcontrib><creatorcontrib>Volkov, V. N.</creatorcontrib><creatorcontrib>Getmanov, Ya. V</creatorcontrib><creatorcontrib>Davidyuk, I. V.</creatorcontrib><creatorcontrib>Deychuly, O. I.</creatorcontrib><creatorcontrib>Dementyev, E. N.</creatorcontrib><creatorcontrib>Dovzhenko, B. A.</creatorcontrib><creatorcontrib>Knyazev, B. A.</creatorcontrib><creatorcontrib>Kolobanov, E. I.</creatorcontrib><creatorcontrib>Kondakov, A. A.</creatorcontrib><creatorcontrib>Kozak, V. R.</creatorcontrib><creatorcontrib>Kozyrev, E. V.</creatorcontrib><creatorcontrib>Kubarev, V. V.</creatorcontrib><creatorcontrib>Kulipanov, G. N.</creatorcontrib><creatorcontrib>Kuper, E. A.</creatorcontrib><creatorcontrib>Kuptsov, I. V.</creatorcontrib><creatorcontrib>Kurkin, G. Ya</creatorcontrib><creatorcontrib>Krutikhin, S. A.</creatorcontrib><creatorcontrib>Medvedev, L. 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A.</creatorcontrib><title>Novosibirsk Free Electron Laser: Recent Achievements and Future Prospects</title><title>Radiophysics and quantum electronics</title><addtitle>Radiophys Quantum El</addtitle><description>Free electron lasers (FELs) are unique sources of electromagnetic radiation with tunable wavelength. A high-power FEL has been created at the G. I.Budker Institute for Nuclear Physics. Its radiation frequency can be tuned over a wide range in the terahertz and infrared spectral ranges. As the source of electron bunches, this FEL uses a multi-turn energy-recovery linac, which has five straight sections. Three sections are used for three FELs which operate in different wavelength ranges (90–240 μm for the first, 37–80 μm for the second, and 5–20 μm for the third ones). The first and the second FELs were commissioned in 2003 and 2009, respectively. They are used for various applied and research problems now. The third FEL is installed on the last, forth accelerator loop, in which the electron energy is the maximum. It comprises three undulator sections and a 40 m optical cavity. The first lasing of this FEL was obtained in the summer of 2015. The radiation wavelength was 9 μm and the average power was about 100 W. The design power is 1 kW at a pulse repetition rate of 3.75 MHz. Radiation of the third FEL will be delivered to user stations from the protected hall in the near future. The third FEL commissioning results are presented and the current status of the first and second FELs as well as their future development prospects are described.</description><subject>Accelerators</subject><subject>Astronomy</subject><subject>Astrophysics and Astroparticles</subject><subject>Electromagnetic radiation</subject><subject>Electromagnetism</subject><subject>Electrons</subject><subject>Free electron lasers</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Infrared</subject><subject>Lasers</subject><subject>Lasing</subject><subject>Mathematical and Computational Physics</subject><subject>Nuclear Physics</subject><subject>Nuclear power generation</subject><subject>Observations and Techniques</subject><subject>Optical Devices</subject><subject>Optics</subject><subject>Photonics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Optics</subject><subject>Spectra</subject><subject>Stations</subject><subject>Theoretical</subject><subject>Wavelengths</subject><issn>0033-8443</issn><issn>1573-9120</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp9kFFLwzAQx4MoOKcfwLc--tKZa9I28W2MTQdDRfQ5pOlldnbNTNqB396M-iyB5Aj_3x33I-QW6AwoLe8DAHBIKZSpLLN4nZEJ5CVLJWT0nEwoZSwVnLNLchXCjtJIcTEh62d3dKGpGh--kpVHTJYtmt67LtnogP4heUODXZ_MzWeDR9zHOiS6q5PV0A8ek1fvwiES4ZpcWN0GvPl7p-RjtXxfPKWbl8f1Yr5JDStonxqkpqprtFBYUzMrtOWaStRVybjWFqzVIEFDbetCYM1ZWRYScssqKjLB2JTcjX0P3n0PGHq1b4LBttUduiEoEJLJ6CGXMTobo1vdomo663qvTTw17hvjOrRN_J9zKQTPcykiACNg4lbBo1UH3-y1_1FA1cmzGj2r2F-dPKvTkGxkQsx2W_Rq5wbfRQX_QL9xgID-</recordid><startdate>2017</startdate><enddate>2017</enddate><creator>Shevchenko, O. 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A high-power FEL has been created at the G. I.Budker Institute for Nuclear Physics. Its radiation frequency can be tuned over a wide range in the terahertz and infrared spectral ranges. As the source of electron bunches, this FEL uses a multi-turn energy-recovery linac, which has five straight sections. Three sections are used for three FELs which operate in different wavelength ranges (90–240 μm for the first, 37–80 μm for the second, and 5–20 μm for the third ones). The first and the second FELs were commissioned in 2003 and 2009, respectively. They are used for various applied and research problems now. The third FEL is installed on the last, forth accelerator loop, in which the electron energy is the maximum. It comprises three undulator sections and a 40 m optical cavity. The first lasing of this FEL was obtained in the summer of 2015. The radiation wavelength was 9 μm and the average power was about 100 W. The design power is 1 kW at a pulse repetition rate of 3.75 MHz. Radiation of the third FEL will be delivered to user stations from the protected hall in the near future. The third FEL commissioning results are presented and the current status of the first and second FELs as well as their future development prospects are described.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s11141-017-9727-9</doi><tpages>8</tpages></addata></record> |
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subjects | Accelerators Astronomy Astrophysics and Astroparticles Electromagnetic radiation Electromagnetism Electrons Free electron lasers Hadrons Heavy Ions Infrared Lasers Lasing Mathematical and Computational Physics Nuclear Physics Nuclear power generation Observations and Techniques Optical Devices Optics Photonics Physics Physics and Astronomy Quantum Optics Spectra Stations Theoretical Wavelengths |
title | Novosibirsk Free Electron Laser: Recent Achievements and Future Prospects |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-03T11%3A06%3A44IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-gale_proqu&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Novosibirsk%20Free%20Electron%20Laser:%20Recent%20Achievements%20and%20Future%20Prospects&rft.jtitle=Radiophysics%20and%20quantum%20electronics&rft.au=Shevchenko,%20O.%20A.&rft.date=2017&rft.volume=59&rft.issue=8-9&rft.spage=605&rft.epage=612&rft.pages=605-612&rft.issn=0033-8443&rft.eissn=1573-9120&rft_id=info:doi/10.1007/s11141-017-9727-9&rft_dat=%3Cgale_proqu%3EA498845598%3C/gale_proqu%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=1893901759&rft_id=info:pmid/&rft_galeid=A498845598&rfr_iscdi=true |