<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Maniscalco, J.T.</author>
             <author>Liepe, M.</author>
             <author>Porter, R.D.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Design Updates on Cavity to Measure Suppression of Microwave Surface Resistance by DC Magnetic Fields
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-191-5</isbn>
		 <electronic-resource-num>10.18429/JACoW-SRF2017-THPB005</electronic-resource-num>
		 <language>English</language>
		 <pages>754-758</pages>
       <pages>THPB005</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>cavity</keyword>
          <keyword>niobium</keyword>
          <keyword>SRF</keyword>
          <keyword>experiment</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2018</year>
          <pub-dates>
             <date>2018-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-SRF2017-THPB005</url>
              <url>http://jacow.org/srf2017/papers/thpb005.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          Our research has shown good agreement between experimental measurements of the anti-Q-slope in niobium SRF cavities and predictions from a recent theoretical model of the suppression of the microwave surface resistance with applied RF field. To confirm that this mechanism is indeed what causes the anti-Q-slope in impurity-doped niobium, it will be necessary to measure the theory's prediction that the same effect may be achieved by applying a constant (i.e. DC) magnetic field parallel to the RF surface. This will also allow for systematic studies of the proposed fundamental effect of the anti-Q-slope and of the behavior of the anti-Q-slope for many surface preparations and alternative materials, since it provides a cleaner measurement by eliminating the counteracting quasiparticle overheating and the complexifying oscillation of the screening currents. In this report we give an update on work at Cornell to design and build a coaxial cavity to measure this effect.
       </abstract>
    </record>
  </records>
</xml>
