<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Lee, T.-Y.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             A Possible Emittance Reduction Scheme for PLSII
          </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-THPOA61</electronic-resource-num>
		 <language>English</language>
		 <pages>1226-1227</pages>
       <pages>THPOA61</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>lattice</keyword>
          <keyword>emittance</keyword>
          <keyword>quadrupole</keyword>
          <keyword>electron</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-THPOA61</url>
              <url>https://jacow.org/napac2016/papers/thpoa61.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          As the upgrade of PLS, PLSII is a 3 GeV light source in 12 super-periods (281.8 m circumference) with 5.8 nm design emittance and can store electron beam up to 400 mA with 3 superconducting RF cavities. PLSII lattice is a double bend achromatic (DBA) lattice with 2 straight sections for each cell (24 straight sections). After comple-tion of PLSII, multi-bend achromatic lattice has widely been adopted to accomplish low emittance. This paper discusses how a minimal change can modify the PLSII's DBA to a quadruple bend achromatic (QBA) lattice and reduce the emittance to about a half value.
       </abstract>
    </record>
  </records>
</xml>
