<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Joo, Y.</author>
             <author>Buaphad, P.</author>
             <author>Cha, S.C.</author>
             <author>Kim, Y.</author>
             <author>Lee, H.R.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Design of 9/6 MeV S-band Electron Linac Structure with 1.5 Bunching Cells
          </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-THPMK139</electronic-resource-num>
		 <language>English</language>
		 <pages>4635-4638</pages>
       <pages>THPMK139</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-THPMK139</url>
              <url>http://jacow.org/ipac2018/papers/thpmk139.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The Korea Atomic Energy Research Institute (KAERI) has been developing several 9/6 MeV dual energy S-band RF electron linear accelerators (linacs) for non-destructive testing such as container inspection system. Until now the bunching cell of the linac has a full-cell geometry. However, to maximize the acceleration of electrons after emission from the electron gun, the geometry of the first bunching cell is modified from a full-cell to a half-cell. The optimization of Q-factor and flatness of electric field along the linac structure can be obtained by adjusting diameters of bunching and power coupling cells. By adjusting gap of the first side-coupling cell, we can optimize the field ratio between the bunching cells and normal accelerating cells. In this paper, we describe design concepts of a 9/6 MeV linac with 1.5 bunching cells as well as optimization of RF parameters such as the quality factor, resonance frequency, and electric field distribution.
       </abstract>
    </record>
  </records>
</xml>
