<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Lee, T.-Y.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Status of PLSII Operation
          </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-THPOA60</electronic-resource-num>
		 <language>English</language>
		 <pages>1223-1225</pages>
       <pages>THPOA60</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>insertion</keyword>
          <keyword>insertion-device</keyword>
          <keyword>impedance</keyword>
          <keyword>operation</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-THPOA60</url>
              <url>https://jacow.org/napac2016/papers/thpoa60.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. Its most unique characteristic is that it has a short straight section and a long straight section for each cell (24 straight sections) and up to 20 insertion devices can be installed. But, as the installed insertion devices, particularly in-vacuum insertion devices, are sources of high impedance, these are quite challenging for high current operation. Current status of PLSII operation and future plans are described in this paper.
       </abstract>
    </record>
  </records>
</xml>
