<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Makita, J.</author>
             <author>Ciovati, G.</author>
             <author>Delayen, J.R.</author>
             <author>Gurevich, A.V.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Cryogenic Probe Station at Old Dominion University Center for Accelerator Science
          </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-MOPB035</electronic-resource-num>
		 <language>English</language>
		 <pages>128-130</pages>
       <pages>MOPB035</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>cavity</keyword>
          <keyword>SRF</keyword>
          <keyword>cryogenics</keyword>
          <keyword>niobium</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-MOPB035</url>
              <url>http://jacow.org/srf2017/papers/mopb035.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          With a growing effort in research and development of an alternative material to bulk Nb for a superconducting radiofrequency (SRF) cavity, it is important to have a cost effective method to benchmark new materials of choice. At Old Dominion University's Center for Accelerator Science, a cryogenic probe station (CPS) will be used to measure the response of superconductor samples under RF fields. The setup consists of a closed-cycle refrigerator for cooling a sample wafer to a cryogenic temperature, a superconducting magnet providing a field parallel to the sample, and DC probes in addition to RF probes. The RF probes will extract a quality factor from a sample patterned in a coplanar waveguide resonator structure on a 2' wafer. From the measured quality factor, the surface resistance and the penetration depth as a function of temperature and magnetic field will be calculated. This paper will discuss the design and measurement procedures of the current CPS setup.
       </abstract>
    </record>
  </records>
</xml>
