<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Guo, J.</author>
             <author>Henry, J.</author>
             <author>Poelker, M.</author>
             <author>Rimmer, R.A.</author>
             <author>Suleiman, R.</author>
             <author>Wang, H.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Using a TE011 Cavity as a Magnetic Momentum Monitor
          </title>
       </titles>
		 <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-201-1</isbn>
		 <electronic-resource-num>10.18429/JACoW-IBIC2018-MOPB17</electronic-resource-num>
		 <language>English</language>
		 <pages>111-113</pages>
       <pages>MOPB17</pages>
       <keywords>
          <keyword>cavity</keyword>
          <keyword>electron</keyword>
          <keyword>GUI</keyword>
          <keyword>impedance</keyword>
          <keyword>coupling</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-IBIC2018-MOPB17</url>
              <url>http://jacow.org/ibic2018/papers/mopb17.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The Jefferson Lab Electron-Ion Collider (JLEIC) design relies on cooling of the ion beam with bunched electron beam constrained in a pair of long solenoids. The high current cooling electron beam needs to be generated in a magnetized electron source, and the beam’s magnetization needs to be maintained during the acceleration and transport to the cooling channel. A non-invasive real time monitoring system is highly desired to quantify electron beam magnetization. The authors propose to use a passive copper RF cavity in TE011 mode as such a monitor. In this paper, we present the mechanism and scaling law of this device, as well as the design and preliminary test results of the prototype cavity.
       </abstract>
    </record>
  </records>
</xml>
