<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Kuriki, M.</author>
             <author>Kashiwagi, S.</author>
             <author>Nagoshi, H.</author>
             <author>Negishi, K.</author>
             <author>Okugi, T.</author>
             <author>Omori, T.</author>
             <author>Satoh, M.</author>
             <author>Seimiya, Y.</author>
             <author>Sumitomo, Y.</author>
             <author>Takahashi, T.</author>
             <author>Urakawa, J.</author>
             <author>Yokoya, K.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             The Effect of Energy Fluctuation on the Multi-bunch Acceleration in E-driven ILC Positron Source
          </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-THPO127</electronic-resource-num>
		 <language>English</language>
		 <pages>958-961</pages>
       <pages>THPO127</pages>
       <keywords>
          <keyword>positron</keyword>
          <keyword>acceleration</keyword>
          <keyword>beam-loading</keyword>
          <keyword>cavity</keyword>
          <keyword>booster</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-THPO127</url>
              <url>http://jacow.org/linac2018/papers/thpo127.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          E-Driven method is a technical backup for positron source for ILC. In the positron source, the positron is generated and accelerated in a multi-bunch format with gaps in a macro-pulse. We employ AM (Amplitude Modulation) to suppress the transient beam-loading, but a small fluctuation is still expected, depending on the compensation accuracy. In this article, the positron yield which is ratio of numbers of positrons over electrons, is evaluated as a function of the compensation accuracy. With this result and the detail investigation of the beam loading compensation accuracy by AM, the positron yield of E-Driven Positron source for ILC is evaluated.
       </abstract>
    </record>
  </records>
</xml>
