<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Checchin, M.</author>
             <author>Grassellino, A.</author>
             <author>Martinello, M.</author>
             <author>Posen, S.</author>
             <author>Romanenko, A.</author>
             <author>Zasadzinski, J.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Enhancement of the Accelerating Gradient in Superconducting Microwave Resonators
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-180-9</isbn>
		 <electronic-resource-num>10.18429/JACoW-NAPAC2016-MOPOB20</electronic-resource-num>
		 <language>English</language>
		 <pages>113-116</pages>
       <pages>MOPOB20</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>cavity</keyword>
          <keyword>induction</keyword>
          <keyword>accelerating-gradient</keyword>
          <keyword>ECR</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-NAPAC2016-MOPOB20</url>
              <url>https://jacow.org/napac2016/papers/mopob20.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The accelerating gradient of superconducting resonators can be enhanced by engineering the thickness of a dirty layer grown at the cavity's rf surface. In this paper the description of the physics behind the accelerating gradient enhancement by meaning of the dirty layer is carried out by solving numerically the the Ginzburg-Landau (GL) equations for the layered system. The calculation shows that the presence of the dirty layer stabilizes the Meissner state up to the lower critical field of the bulk, increasing the maximum accelerating gradient.
       </abstract>
    </record>
  </records>
</xml>
