<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Goryashko, V.A.</author>
             <author>Dancila, D.S.</author>
             <author>Gajewski, K.J.</author>
             <author>Hermansson, L.</author>
             <author>Li, H.</author>
             <author>Nicander, H.</author>
             <author>Ruber, R.J.M.Y.</author>
             <author>Santiago Kern, R.</author>
             <author>Teerikoski, S.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             High-Precision Measurements of the Quality Factor of Superconducting Cavities at the FREIA Laboratory
          </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-TUPB089</electronic-resource-num>
		 <language>English</language>
		 <pages>810-813</pages>
       <pages>TUPB089</pages>
       <keywords>
          <keyword>cavity</keyword>
          <keyword>coupling</keyword>
          <keyword>impedance</keyword>
          <keyword>network</keyword>
          <keyword>SRF</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-TUPB089</url>
              <url>http://srf2015.vrws.de/papers/tupb089.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          In this paper we propose a high-precision method of measuring Q0 of SRF cavities. A common way to study the performance of an SRF cavity is to build an oscillator around it that is referred to as a self-exciting loop. In the standard approach, by tuning the loop phase for a maximum field level in the cavity and measuring forward and reflected waves, one finds the cavity coupling. Then, performing a time-decay measurement and finding the total quality factor, one gets Q0. However, this approach suffers from a deficiency originating from a single data-point measurement of the reflection coefficient. In our method by varying the loop phase shift, one obtains amplitudes of the reflection coefficient of the cavity as a function of its phases. The complex reflection coefficient describes a perfect circle in polar coordinates. Fitting the overdetermined set of data to that circle allows more accurate calculation of Q0 via the least-squares procedure. The method has been tested at the FREIA Laboratory on two cavities from IPN Orsay: a single spoke and a prototype ESS double spoke.
       </abstract>
    </record>
  </records>
</xml>
