<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Xiao, A.</author>
             <author>Borland, M.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Beam Loss Simulation and Collimator System Configurations for the Advanced Photon Source Upgrade
          </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-WEPOB22</electronic-resource-num>
		 <language>English</language>
		 <pages>943-945</pages>
       <pages>WEPOB22</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>simulation</keyword>
          <keyword>beam-losses</keyword>
          <keyword>shielding</keyword>
          <keyword>injection</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-WEPOB22</url>
              <url>https://jacow.org/napac2016/papers/wepob22.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The proposed multi-bend achromat lattice for the Advanced Photon Source upgrade (APS-U) has a design emittance of less than 70 pm. The Touschek loss rate is high: compared with the current APS ring, which has an average beam lifetime  ∼  10 h, the simulated beam lifetime for APS-U is only ~2 h when operated in the high flux mode (I=200 mA in 48 bunches). An additional consequence of the short lifetime is that injection must be more frequent, which provides another potential source of particle loss. In order to provide information for the radiation shielding system evaluation and to avoid particle loss in sensitive locations around the ring (for example, insertion device straight sections), simulations of the detailed beam loss distribution have been performed. Several possible collimation configurations have been simulated and compared.
       </abstract>
    </record>
  </records>
</xml>
