<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Kolb, P.</author>
             <author>Laxdal, R.E.</author>
             <author>Ma, Y.</author>
             <author>Yao, Z.Y.</author>
             <author>Zvyagintsev, V.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             HOM Measurements on the ARIEL eLINAC Cryomodules
          </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-MOPB088</electronic-resource-num>
		 <language>English</language>
		 <pages>347-349</pages>
       <pages>MOPB088</pages>
       <keywords>
          <keyword>HOM</keyword>
          <keyword>cavity</keyword>
          <keyword>simulation</keyword>
          <keyword>cryomodule</keyword>
          <keyword>linac</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-MOPB088</url>
              <url>http://srf2015.vrws.de/papers/mopb088.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The ARIEL eLINAC is a 50 MeV, 10 mA electron LINAC designed for the creation of rare isotopes via photo-fission. Future upgrade plans include the addition of a recirculating beam line to allow for either further energy increase of the beam beyond 50 MeV or to operate a free electron laser in an energy recovery mode. For both recirculating LINAC and ERL the higher order modes (HOM) have to be sufficiently suppressed to prevent beam-break-up. The design of the 1.3 GHz nine-cell cavity incorporated this requirement by including beam line absorbers on both ends of each cavity and an asymmetric beam pipe configuration on the cavity to allow trapped modes to propagate to the beam line absorbers. Measurements of the higher order modes on the completed injector cryomodule and the first cavity in the accelerating cryomodules will be shown and compared to simulations.
       </abstract>
    </record>
  </records>
</xml>
