<?xml version="1.0" encoding="UTF-8"?>
<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Feng, B.Y.</author>
             <author>Chen, H.B.</author>
             <author>Gao, Q.</author>
             <author>Lin, X.</author>
             <author>Shi, J.R.</author>
             <author>Zha, H.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Multipole Field Optimization of X-Band High Gradient Structure
          </title>
       </titles>
       <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-265-3</isbn>
		 <electronic-resource-num>10.18429/JACoW-SAP2023-TUPB013</electronic-resource-num>
		 <language>English</language>
		 <pages>108-110</pages>
       <keywords>
          <keyword>multipole</keyword>
          <keyword>quadrupole</keyword>
          <keyword>cavity</keyword>
          <keyword>simulation</keyword>
          <keyword>acceleration</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2024</year>
          <pub-dates>
             <date>2024-11</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-SAP2023-TUPB013</url>
              <url>https://jacow.org/sap2023/papers/tupb013.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The X-band constant gradient acceleration structure plays a crucial role in the VIGAS project. However, the presence of a multipole field component in the struc-ture’s coupler leads to an increase in ray bandwidth and a decrease in yield, ultimately affecting the quality of the generated rays. Through calculations, it has been determined that the quadrupole field component is particularly prominent in the original structure, ac-counting for 29.5\% of the fundamental mode strength. Therefore, it is necessary to modify the cavity struc-ture of the coupler. By altering the shape of the cavity to two staggered circles, the objective of reducing the quadrupole field is achieved. The optimized quadru-pole field component now accounts for approximately 0.3\% of the fundamental mode strength. Subsequently, the non-resonant perturbation method was employed to simulate and experimentally measure the magnitude of the multipole field component in the actual acceler-ation cavity.
       </abstract>
    </record>
  </records>
</xml>
