<?xml version="1.0" encoding="UTF-8"?>
<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Huang, W.L.</author>
             <author>Liu, M.Y.</author>
             <author>Liu, Q.R.</author>
             <author>Liu, X.Y.</author>
             <author>Nie, X.J.</author>
             <author>Sui, Y.F.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Design and Test of a Prototype 324 MHz RF Deflector in the Bunch Shape Monitor for CSNS-II Linac Upgrade
          </title>
       </titles>
       <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>2673-5350</isbn>
		 <isbn>978-3-95450-236-3</isbn>
		 <electronic-resource-num>10.18429/JACoW-IBIC2023-TUP014</electronic-resource-num>
		 <language>English</language>
		 <pages>219-221</pages>
       <keywords>
          <keyword>linac</keyword>
          <keyword>electron</keyword>
          <keyword>cavity</keyword>
          <keyword>proton</keyword>
          <keyword>neutron</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2023</year>
          <pub-dates>
             <date>2023-12</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-IBIC2023-TUP014</url>
              <url>https://jacow.org/ibic2023/papers/tup014.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          During the upgrade of linac in CSNS-II, the beam in-jection energy will increase from 80.1MeV to 300MeV and the beam power from 100kW to 500kW. A com-bined layout of superconducting spoke cavities and ellip-tical cavities is adopted to accelerate H⁻ beam to 300MeV. Due to a ~10ps short bunch width at the exit of the spoke SC section, the longitudinal beam density dis-tribution will be measured by bunch shape monitors using low energy secondary emission electrons. As the most important part of a bunch shape monitor, a prototype 324MHz RF deflector is designed and tuned on the basis of a quasi-symmetric λ/2 325MHz coaxial resona-tor, which was fabricated for the C-ADS proton accelera-tor project. Preliminary parameters of the bunch shape monitor are presented. Simulation of the RF deflector and test results in the laboratory are described and analysed.
       </abstract>
    </record>
  </records>
</xml>
