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Localization of rf breakdowns in a standing wave cavity
At SLAC, a five-cell, normal-conducting, L -band (1.3 GHz), standing-wave (SW) cavity was built as a prototype positron capture accelerator for the ILC. The structure met the ILC gradient goal but required extensive rf processing. When rf breakdowns occurred, a large variation was observed in the de...
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Published in: | Physical review special topics. PRST-AB. Accelerators and beams 2009-04, Vol.12 (4), p.042001, Article 042001 |
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description | At SLAC, a five-cell, normal-conducting, L -band (1.3 GHz), standing-wave (SW) cavity was built as a prototype positron capture accelerator for the ILC. The structure met the ILC gradient goal but required extensive rf processing. When rf breakdowns occurred, a large variation was observed in the decay rate of the stored energy in the cavity after the input power was shut off. It appeared that the breakdowns were isolating sections of the cavity, and that the trapped energy in those sections was then partitioned among its natural modes, producing a distinct beating pattern during the decay. To explore this phenomenon further, an equivalent circuit model of cavity was created that reproduces well its normal operating characteristics. The model was then used to compute the spectra of trapped energy for different numbers of isolated cells. The resulting modal patterns agree well with those of the breakdown data, and thus such a comparison appears to provide a means of identifying the irises on which the breakdowns occurred. |
doi_str_mv | 10.1103/PhysRevSTAB.12.042001 |
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The structure met the ILC gradient goal but required extensive rf processing. When rf breakdowns occurred, a large variation was observed in the decay rate of the stored energy in the cavity after the input power was shut off. It appeared that the breakdowns were isolating sections of the cavity, and that the trapped energy in those sections was then partitioned among its natural modes, producing a distinct beating pattern during the decay. To explore this phenomenon further, an equivalent circuit model of cavity was created that reproduces well its normal operating characteristics. The model was then used to compute the spectra of trapped energy for different numbers of isolated cells. 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PRST-AB. Accelerators and beams</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wang, Faya</au><au>Adolphsen, Chris</au><aucorp>SLAC National Accelerator Lab., Menlo Park, CA (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Localization of rf breakdowns in a standing wave cavity</atitle><jtitle>Physical review special topics. PRST-AB. Accelerators and beams</jtitle><date>2009-04-01</date><risdate>2009</risdate><volume>12</volume><issue>4</issue><spage>042001</spage><pages>042001-</pages><artnum>042001</artnum><issn>1098-4402</issn><eissn>1098-4402</eissn><eissn>2469-9888</eissn><abstract>At SLAC, a five-cell, normal-conducting, L -band (1.3 GHz), standing-wave (SW) cavity was built as a prototype positron capture accelerator for the ILC. The structure met the ILC gradient goal but required extensive rf processing. 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subjects | ACCELERATORS Accelerators,ACCPHY BREAKDOWN DECAY Decay rate EQUIVALENT CIRCUITS Internal energy PARTICLE ACCELERATORS POSITRONS PROCESSING SPECTRA STANDING WAVES STANFORD LINEAR ACCELERATOR CENTER STORED ENERGY |
title | Localization of rf breakdowns in a standing wave cavity |
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