<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Conway, Z.A.</author>
             <author>Guilfoyle, B.M.</author>
             <author>Guo, H.</author>
             <author>Kedzie, M.</author>
             <author>Kelly, M.P.</author>
             <author>Reid, T.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Progress Toward 2 K High Performance Half-wave Resonators and Cryomodule
          </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-WEYA05</electronic-resource-num>
		 <language>English</language>
		 <pages>692-694</pages>
       <pages>WEYA05</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>cavity</keyword>
          <keyword>cryomodule</keyword>
          <keyword>cryogenics</keyword>
          <keyword>SRF</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-WEYA05</url>
              <url>http://jacow.org/srf2017/papers/weya05.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          Argonne National Laboratory is implementing a novel 2.0 K superconducting cavity cryomodule operating at 162.5 MHz. This cryomodule is designed for the acceleration of 2 mA H-/proton beams from 2.1 to 10.3 MeV as part of the Fermilab Proton Improvement Project-II (PIP-II). The 2.0 K cryomodule is comprised of 8 half-wave cavities operated in the continuous wave mode with 8 superconducting magnets, one in front of each cavity. In this paper we will review recent cavity results which demonstrate continuous-wave operated cavities with low-field residual resistances of 2.5 nΩ which achieve peak surface fields up to 134 MV/m and 144 mT, electric and magnetic respectively, with field emission onset fields greater than 70 MV/m in the production cavities following the prototyping effort.
       </abstract>
    </record>
  </records>
</xml>
