<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Ji, Y.</author>
             <author>Spentzouris, L.K.</author>
             <author>Zwaska, R.M.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             POSINST Simulation on Fermilab Main Injector and Recycler Ring
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-180-9</isbn>
		 <electronic-resource-num>10.18429/JACoW-NAPAC2016-TUPOB63</electronic-resource-num>
		 <language>English</language>
		 <pages>632-635</pages>
       <pages>TUPOB63</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>electron</keyword>
          <keyword>dipole</keyword>
          <keyword>simulation</keyword>
          <keyword>proton</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-NAPAC2016-TUPOB63</url>
              <url>https://jacow.org/napac2016/papers/tupob63.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The Fermilab accelerator complex is currently undergoing an upgrade from 400kW to 700kW. This intensity could push operations into the region where electron cloud (e-cloud) generation could be observed and even cause instabilities. The POSINST simulation code was used to study how in- creasing beam intensities will affect electron cloud genera- tion. Threshold simulations show how the e-cloud density depend on the beam intensity and secondary electron yield (SEY) in the Main Injector (MI) and Recycler Ring (RR).
       </abstract>
    </record>
  </records>
</xml>
