The Klynac: An integrated klystron and linear accelerator
The Klynac concept integrates an electron gun, a radio frequency (RF) power source, and a coupled-cavity linear accelerator into a single resonant system. The klystron is essentially a conventional klystron structure with an input cavity, some number of intermediate cavities and an output cavity. Th...
Gespeichert in:
Veröffentlicht in: | AIP conference proceedings 2013-04, Vol.1525 (1) |
---|---|
Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | |
---|---|
container_issue | 1 |
container_start_page | |
container_title | AIP conference proceedings |
container_volume | 1525 |
creator | Potter, James M Schwellenbach, David Meidinger, Alfred |
description | The Klynac concept integrates an electron gun, a radio frequency (RF) power source, and a coupled-cavity linear accelerator into a single resonant system. The klystron is essentially a conventional klystron structure with an input cavity, some number of intermediate cavities and an output cavity. The accelerator structure is, likewise, a conventional on-axis coupled structure. The uniqueness is the means of coupling the klystron output cavity to the accelerator. The coupler is a resonant coupler rather than an ordinary transmission line. The geometry of such a system need not be coaxial. However, if the klystron and accelerator are coaxial we can eliminate the need for a separate cathode for the accelerator by injecting some of the klystron beam into the accelerator. Such a device can be made cylindrical which is ideal for some applications. |
doi_str_mv | 10.1063/1.4802315 |
format | Article |
fullrecord | <record><control><sourceid>proquest_osti_</sourceid><recordid>TN_cdi_osti_scitechconnect_22116955</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>1660054156</sourcerecordid><originalsourceid>FETCH-LOGICAL-c291t-4ebc7e9487cffe3f4f329543559f9f84b9c12477f3b09d33d38c575fafe4b66a3</originalsourceid><addsrcrecordid>eNotkDtPwzAUhS0eElXpwD-IxMKScu3rR8xWVbxEJZYisUWOc00DwYHYHfrviVSmM5xPR58OY1cclhw03vKlrEAgVydsxpXipdFcn7KFNRUYVJJzWZkzNgOwshQS3y_YIqVPABCAQliYMbvdUfHSH6Lzd8UqFl3M9DG6TG3x1R9SHodYuNgWfRfJjYXznnqa-mG8ZOfB9YkW_zlnbw_32_VTuXl9fF6vNqUXludSUuMN2UnEh0AYZEBhlUSlbLChko31XEhjAjZgW8QWK6-MCi6QbLR2OGfXx90h5a5Ovsvkd36IkXyuheBcW6Um6uZI_YzD755Srr-7NLn2LtKwTzXXGmB6RGn8AwulWFk</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>1660054156</pqid></control><display><type>article</type><title>The Klynac: An integrated klystron and linear accelerator</title><source>AIP Journals Complete</source><creator>Potter, James M ; Schwellenbach, David ; Meidinger, Alfred</creator><creatorcontrib>Potter, James M ; Schwellenbach, David ; Meidinger, Alfred</creatorcontrib><description>The Klynac concept integrates an electron gun, a radio frequency (RF) power source, and a coupled-cavity linear accelerator into a single resonant system. The klystron is essentially a conventional klystron structure with an input cavity, some number of intermediate cavities and an output cavity. The accelerator structure is, likewise, a conventional on-axis coupled structure. The uniqueness is the means of coupling the klystron output cavity to the accelerator. The coupler is a resonant coupler rather than an ordinary transmission line. The geometry of such a system need not be coaxial. However, if the klystron and accelerator are coaxial we can eliminate the need for a separate cathode for the accelerator by injecting some of the klystron beam into the accelerator. Such a device can be made cylindrical which is ideal for some applications.</description><identifier>ISSN: 0094-243X</identifier><identifier>ISBN: 9780735411487</identifier><identifier>ISBN: 0735411484</identifier><identifier>EISSN: 1551-7616</identifier><identifier>DOI: 10.1063/1.4802315</identifier><language>eng</language><publisher>United States</publisher><subject>Accelerators ; CATHODES ; CYLINDRICAL CONFIGURATION ; Devices ; ELECTRON GUNS ; Holes ; INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY ; Joining ; KLYSTRONS ; LINEAR ACCELERATORS ; PARTICLE ACCELERATORS ; PARTICLE BEAMS ; Radio frequencies ; RF SYSTEMS ; Uniqueness</subject><ispartof>AIP conference proceedings, 2013-04, Vol.1525 (1)</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c291t-4ebc7e9487cffe3f4f329543559f9f84b9c12477f3b09d33d38c575fafe4b66a3</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22116955$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Potter, James M</creatorcontrib><creatorcontrib>Schwellenbach, David</creatorcontrib><creatorcontrib>Meidinger, Alfred</creatorcontrib><title>The Klynac: An integrated klystron and linear accelerator</title><title>AIP conference proceedings</title><description>The Klynac concept integrates an electron gun, a radio frequency (RF) power source, and a coupled-cavity linear accelerator into a single resonant system. The klystron is essentially a conventional klystron structure with an input cavity, some number of intermediate cavities and an output cavity. The accelerator structure is, likewise, a conventional on-axis coupled structure. The uniqueness is the means of coupling the klystron output cavity to the accelerator. The coupler is a resonant coupler rather than an ordinary transmission line. The geometry of such a system need not be coaxial. However, if the klystron and accelerator are coaxial we can eliminate the need for a separate cathode for the accelerator by injecting some of the klystron beam into the accelerator. Such a device can be made cylindrical which is ideal for some applications.</description><subject>Accelerators</subject><subject>CATHODES</subject><subject>CYLINDRICAL CONFIGURATION</subject><subject>Devices</subject><subject>ELECTRON GUNS</subject><subject>Holes</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><subject>Joining</subject><subject>KLYSTRONS</subject><subject>LINEAR ACCELERATORS</subject><subject>PARTICLE ACCELERATORS</subject><subject>PARTICLE BEAMS</subject><subject>Radio frequencies</subject><subject>RF SYSTEMS</subject><subject>Uniqueness</subject><issn>0094-243X</issn><issn>1551-7616</issn><isbn>9780735411487</isbn><isbn>0735411484</isbn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNotkDtPwzAUhS0eElXpwD-IxMKScu3rR8xWVbxEJZYisUWOc00DwYHYHfrviVSmM5xPR58OY1cclhw03vKlrEAgVydsxpXipdFcn7KFNRUYVJJzWZkzNgOwshQS3y_YIqVPABCAQliYMbvdUfHSH6Lzd8UqFl3M9DG6TG3x1R9SHodYuNgWfRfJjYXznnqa-mG8ZOfB9YkW_zlnbw_32_VTuXl9fF6vNqUXludSUuMN2UnEh0AYZEBhlUSlbLChko31XEhjAjZgW8QWK6-MCi6QbLR2OGfXx90h5a5Ovsvkd36IkXyuheBcW6Um6uZI_YzD755Srr-7NLn2LtKwTzXXGmB6RGn8AwulWFk</recordid><startdate>20130419</startdate><enddate>20130419</enddate><creator>Potter, James M</creator><creator>Schwellenbach, David</creator><creator>Meidinger, Alfred</creator><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20130419</creationdate><title>The Klynac: An integrated klystron and linear accelerator</title><author>Potter, James M ; Schwellenbach, David ; Meidinger, Alfred</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c291t-4ebc7e9487cffe3f4f329543559f9f84b9c12477f3b09d33d38c575fafe4b66a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Accelerators</topic><topic>CATHODES</topic><topic>CYLINDRICAL CONFIGURATION</topic><topic>Devices</topic><topic>ELECTRON GUNS</topic><topic>Holes</topic><topic>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</topic><topic>Joining</topic><topic>KLYSTRONS</topic><topic>LINEAR ACCELERATORS</topic><topic>PARTICLE ACCELERATORS</topic><topic>PARTICLE BEAMS</topic><topic>Radio frequencies</topic><topic>RF SYSTEMS</topic><topic>Uniqueness</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Potter, James M</creatorcontrib><creatorcontrib>Schwellenbach, David</creatorcontrib><creatorcontrib>Meidinger, Alfred</creatorcontrib><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>AIP conference proceedings</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Potter, James M</au><au>Schwellenbach, David</au><au>Meidinger, Alfred</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Klynac: An integrated klystron and linear accelerator</atitle><jtitle>AIP conference proceedings</jtitle><date>2013-04-19</date><risdate>2013</risdate><volume>1525</volume><issue>1</issue><issn>0094-243X</issn><eissn>1551-7616</eissn><isbn>9780735411487</isbn><isbn>0735411484</isbn><abstract>The Klynac concept integrates an electron gun, a radio frequency (RF) power source, and a coupled-cavity linear accelerator into a single resonant system. The klystron is essentially a conventional klystron structure with an input cavity, some number of intermediate cavities and an output cavity. The accelerator structure is, likewise, a conventional on-axis coupled structure. The uniqueness is the means of coupling the klystron output cavity to the accelerator. The coupler is a resonant coupler rather than an ordinary transmission line. The geometry of such a system need not be coaxial. However, if the klystron and accelerator are coaxial we can eliminate the need for a separate cathode for the accelerator by injecting some of the klystron beam into the accelerator. Such a device can be made cylindrical which is ideal for some applications.</abstract><cop>United States</cop><doi>10.1063/1.4802315</doi><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0094-243X |
ispartof | AIP conference proceedings, 2013-04, Vol.1525 (1) |
issn | 0094-243X 1551-7616 |
language | eng |
recordid | cdi_osti_scitechconnect_22116955 |
source | AIP Journals Complete |
subjects | Accelerators CATHODES CYLINDRICAL CONFIGURATION Devices ELECTRON GUNS Holes INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY Joining KLYSTRONS LINEAR ACCELERATORS PARTICLE ACCELERATORS PARTICLE BEAMS Radio frequencies RF SYSTEMS Uniqueness |
title | The Klynac: An integrated klystron and linear accelerator |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-05T05%3A54%3A33IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_osti_&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=The%20Klynac:%20An%20integrated%20klystron%20and%20linear%20accelerator&rft.jtitle=AIP%20conference%20proceedings&rft.au=Potter,%20James%20M&rft.date=2013-04-19&rft.volume=1525&rft.issue=1&rft.issn=0094-243X&rft.eissn=1551-7616&rft.isbn=9780735411487&rft.isbn_list=0735411484&rft_id=info:doi/10.1063/1.4802315&rft_dat=%3Cproquest_osti_%3E1660054156%3C/proquest_osti_%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=1660054156&rft_id=info:pmid/&rfr_iscdi=true |