<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Nagoshi, H.</author>
             <author>Kashiwagi, S.</author>
             <author>Kuriki, M.</author>
             <author>Negishi, K.</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>
          </authors>
       </contributors>
       <titles>
          <title>
             A Design Study of the Electron-driven ILC Positron Source Including Beam Loading Effect
          </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-MOPMF077</electronic-resource-num>
		 <language>English</language>
		 <pages>311-314</pages>
       <pages>MOPMF077</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-MOPMF077</url>
              <url>http://jacow.org/ipac2018/papers/mopmf077.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The International Linear Collider (ILC) is a next-generation accelerator for high-energy physics to study the Higgs and top sector in the Standard Model, and new physics such as supersymmetry and dark matter. ILC positron source based on Electron-driven method has been proposed as a reliable technical backup. In this article, we report the design study of the positron source based on the off-the-shelf RF components. The positron is generated and accelerated in a multi-bunch format. To compensate the energy variation by the transient beam loading effect, we employ AM (Amplitude Modulation) technique and the results were 16.60 ± 0.14 MV (peak-to-peak) for L-band 2m cavity driven by 22.5 MW power and 25.76 ± 0.19 MV (peak-to-peak) for S-band 2m ac-celerator driven by 36 MW power with 0.78 A beam load-ing.
       </abstract>
    </record>
  </records>
</xml>
