<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Welander, P.B.</author>
             <author>Franzi, M.A.</author>
             <author>Tantawi, S.G.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Cryogenic RF Characterization of Superconducting Materials at SLAC With Hemispherical Cavities
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-178-6</isbn>
		 <electronic-resource-num>10.18429/JACoW-SRF2015-TUPB065</electronic-resource-num>
		 <language>English</language>
		 <pages>735-738</pages>
       <pages>TUPB065</pages>
       <keywords>
          <keyword>cavity</keyword>
          <keyword>niobium</keyword>
          <keyword>SRF</keyword>
          <keyword>factory</keyword>
          <keyword>cryogenics</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2015</year>
          <pub-dates>
             <date>2015-12</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-SRF2015-TUPB065</url>
              <url>http://srf2015.vrws.de/papers/tupb065.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          For the characterization of SRF materials, we have commissioned a second-generation, X-band cavity cryostat that can rapidly analyze thin-film coatings or bulk samples. The system operates at 11.4 GHz, at temperatures down to 4 K, and utilizes two interchangeable hemispherical cavities (one Cu, one Nb) that can accommodate 51 mm-diameter samples on the flat side. The cavities are designed to operate with a TE032-like mode where the magnetic field is strongest on the sample surface. As a result, the sample accounts for 33% of the overall cavity loss, despite comprising less than 8% of the total surface area. For low-power testing we utilize a programmable network analyzer, while for high-power testing we connect the cavity to a 50 MW XL-4 klystron. With the Nb cavity we can measure surface resistances down to 0.7 microhm, while with the Cu cavity we can measure quenching fields up to 360 mT. X-band operation permits a compact cavity and cryostat design with a reasonable sample size, while the closed-cycle pulse-tube cryorefrigerator allows for rapid sample cycling. We will discuss cryostat design, cavity modeling, measurement limits, and recent sample testing results.
       </abstract>
    </record>
  </records>
</xml>
