<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Maniscalco, J.T.</author>
             <author>Ge, M.</author>
             <author>Gonnella, D.</author>
             <author>Liepe, M.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Investigation of the Origin of the Anti-Q-Slope
          </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-MOPOB65</electronic-resource-num>
		 <language>English</language>
		 <pages>218-220</pages>
       <pages>MOPOB65</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>cavity</keyword>
          <keyword>ECR</keyword>
          <keyword>experiment</keyword>
          <keyword>SRF</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-MOPOB65</url>
              <url>https://jacow.org/napac2016/papers/mopob65.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The surface resistance of a superconductor, a property very relevant to SRF accelerators, has long been known to depend on the strength of the surface magnetic field. A recent discovery showed that, for certain surface treatments, microwave cavities can be shown to have an inverse field dependence, dubbed the ‘‘anti-Q-slope'', in which the surface resistance decreases over an increasing field. Here we present an investigation into what causes the anti-Q-slope in nitrogen-doped niobium cavities, drawing a direct connection between the electron mean free path of the SRF material and the magnitude of the anti-Q-slope. Further, we incorporate residual resistance due to flux trapping to calculate an optimal mean free path for a given trapped flux.
       </abstract>
    </record>
  </records>
</xml>
