<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Ge, M.</author>
             <author>Gonnella, D.</author>
             <author>Liepe, M.</author>
             <author>Sears, J.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Cool Down Studies for the LCLS-II Project
          </title>
       </titles>
		 <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>2226-0366</isbn>
		 <isbn>978-3-95450-194-6</isbn>
		 <electronic-resource-num>10.18429/JACoW-LINAC2018-TUPO058</electronic-resource-num>
		 <language>English</language>
		 <pages>470-472</pages>
       <pages>TUPO058</pages>
       <keywords>
          <keyword>cavity</keyword>
          <keyword>network</keyword>
          <keyword>SRF</keyword>
          <keyword>cryomodule</keyword>
          <keyword>linac</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2019</year>
          <pub-dates>
             <date>2019-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-LINAC2018-TUPO058</url>
              <url>http://jacow.org/linac2018/papers/tupo058.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The quality factor of the nitrogen-doped SRF cavities for the LCLS-II project are strongly impacted by cool down speed. A sufficiently fast cool down speed can produce large thermal gradient across a cavity and sufficiently expel magnetic flux when the cavity wall passes from the normal-conducting to the superconducting state. However, instrumentation in LCLS-II production cryomodules has been kept at a minimum, and additional information during the cool down of the modules is therefore desirable. In this work, we study if and how RF data can be used during cavity cool-down to determine the transition speeds of the individual cavities in the LCLS-II linac.
       </abstract>
    </record>
  </records>
</xml>
