<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Neveu, N.R.</author>
             <author>Gai, W.</author>
             <author>Jing, C.-J.</author>
             <author>Power, J.G.</author>
             <author>Spentzouris, L.K.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Staged Two Beam Acceleration Beam Line Design for the AWA Facility
          </title>
       </titles>
		 <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-184-7</isbn>
		 <electronic-resource-num>10.18429/JACoW-IPAC2018-TUPML064</electronic-resource-num>
		 <language>English</language>
		 <pages>1688-1691</pages>
       <pages>TUPML064</pages>
       <keywords>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2018</year>
          <pub-dates>
             <date>2018-06</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-IPAC2018-TUPML064</url>
              <url>http://jacow.org/ipac2018/papers/tupml064.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          Two beam acceleration is a candidate for future high energy physics machines and FEL user facilities. This scheme consists of two independent electron beam lines operating synchronously. High-charge, 70 MeV drive bunch trains are injected from the RF photo-injector into decelerating structures to generate a few hundred of MW of RF power. This RF power is transferred through an RF waveguide to accelerating structures that are used to accelerate the witness beam. Staging refers to the sequential acceleration (energy gain) in two or more structures on the witness beam line. A kicker was incorporated on the drive beam line to accomplish a modular design so that each accelerating structure can be independently powered by a separate drive beam. Simulations were performed in OPAL-T to model the two beam lines. Beam sizes at the center of the structures was minimized to ensure good charge transmission. The resulting design will be the basis for proof of principle experiments that will take place at the Argonne Wakefield Accelerator (AWA) facility.
       </abstract>
    </record>
  </records>
</xml>
