<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Bazyl, D.B.</author>
             <author>De Gersem, H.</author>
             <author>MÃ¼ller, W.F.O.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Upgrade of the Capture Section of the S-DALINAC Injector
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-182-3</isbn>
		 <electronic-resource-num>10.18429/JACoW-IPAC2017-MOPVA055</electronic-resource-num>
		 <language>English</language>
		 <pages>993-995</pages>
       <pages>MOPVA055</pages>
       <keywords>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-05</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-IPAC2017-MOPVA055</url>
              <url>http://jacow.org/ipac2017/papers/mopva055.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          In order to reduce the energy spread of the recirculated beam, the injector of the S-DALINAC needs to be optimized, because the non-isochronous recirculation cannot correct for errors originating from the injector linac. For the S-DALINAC, spatial restrictions suggest the use of SRF technology for the capture section. In this work, we consider various SRF cavities with an operating frequency of 3 GHz for a possible upgrade of the capture section of the S-DALINAC. The first results of the RF and beam dynamics simulations for the proposed options are presented in this paper.
       </abstract>
    </record>
  </records>
</xml>
