<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Calatroni, S.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             HTS Coatings for Impedance Reduction of Beam-Induced RF Image Currents in the FCC
          </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-TUPB052</electronic-resource-num>
		 <language>English</language>
		 <pages>695-699</pages>
       <pages>TUPB052</pages>
       <keywords>
          <keyword>impedance</keyword>
          <keyword>radiation</keyword>
          <keyword>collider</keyword>
          <keyword>dipole</keyword>
          <keyword>injection</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-TUPB052</url>
              <url>http://srf2015.vrws.de/papers/tupb052.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The FCC-hh presently under study at CERN will make use of 16 T superconducting dipoles for achieving 100 TeV p-p center-of-mass collision energy in a 100 km ring collider. A copper coated beam screen, like in the LHC, is envisaged to shield the 1.9 K dipole cold bores from the 28 W/m/beam of synchrotron radiation. Operating temperature should be in the 50 K range, as best compromise temperature in order to minimize the wall-plug power consumption of the cryogenic system. However, preliminary studies indicate that copper at 50 K might not provide low enough beam coupling impedance in the FCC-hh. It has then been proposed to reduce the beam impedance by a thin layer of a High-Temperature Superconductor (HTS), which will thus effectively shield the beam-induced RF image currents. Purpose of this paper is to define the basic requirements for an HTS film in the RF field induced by beam image currents and exposed to a high magnetic field, and to identify the best candidate materials and coating processes.
       </abstract>
    </record>
  </records>
</xml>
