<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Du, H.</author>
             <author>Kong, Q.Y.</author>
             <author>Li, Z.S.</author>
             <author>Wang, K.D.</author>
             <author>Yin, X.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             RF Design and Cold Model Measurement of an IH-DTL for HIMM Injector
          </title>
       </titles>
		 <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>2226-0366</isbn>
		 <isbn>978-3-95450-194-6</isbn>
		 <electronic-resource-num>10.18429/JACoW-LINAC2018-TUPO004</electronic-resource-num>
		 <language>English</language>
		 <pages>329-331</pages>
       <pages>TUPO004</pages>
       <keywords>
          <keyword>DTL</keyword>
          <keyword>cavity</keyword>
          <keyword>linac</keyword>
          <keyword>simulation</keyword>
          <keyword>quadrupole</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2019</year>
          <pub-dates>
             <date>2019-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-LINAC2018-TUPO004</url>
              <url>http://jacow.org/linac2018/papers/tupo004.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          An interdigital H-mode drift tube linac (IH-DTL) will be constructed as a postinjector linac for the Heavy Ion Medical Machine (HIMM). Its resonant frequency, injec-tion and final energies are determined from beam dynamics and hardware parameters considerations of the entire machine to be 162.5MHz, 600keV/u and 4MeV/u, respectively. The beam duty cycle of the injector linac is less than 0.1% based on the injection requirements of the synchrotron. Beam dynamics and RF structure design and optimize of the IH-DTL has been finished. The maximum surface electric field is less than 2.0-times the Kilpatric limit for accelerating C⁴⁺ beam. This IH-DTL contains 42 accelerating gaps and two focusing quadrupole triplets. In order to examine the field distribution of the IH-DTL which reaches the length of 3.17m, an aluminum alloy 1:1 cold model cavity with 4 moveable tuners and 2 empty focusing magnet shell was constructed. The relative intertube-distance errors are less than ±50μm. The measurements show that the gap voltage values can match the CST-MWS simulating results within relative difference of ±3% by adjusting the 4 moveable tuners.
       </abstract>
    </record>
  </records>
</xml>
