<?xml version="1.0" encoding="UTF-8"?>
<articles>
<article xmlns:xlink="http://www.w3.org/1999/xlink/">
  <front>
    <journal-meta>
      <journal-title>IEEE Trans. Nucl. Sci.</journal-title>
      <abbrev-journal-title>IEEE Trans. Nucl. Sci.</abbrev-journal-title>
      <issn>0018-9499</issn>
    </journal-meta>
    <article-meta>
      <title-group>
        <article-title>Single- and double-drift bunchers as possible injection schemes for the CPS linac</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name>
            <surname>Bru</surname>
            <given-names>B</given-names>
          </name>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Weiss</surname>
            <given-names>M</given-names>
          </name>
        </contrib>
      </contrib-group>
      <pub-date pub-type="pub">
        <year>1973</year>
      </pub-date>
      <volume>20</volume>
      <fpage>963</fpage>
      <lpage>5</lpage>
      <self-uri xlink:href="http://cds.cern.ch/record/955538"/>
      <self-uri xlink:href="http://preprints.cern.ch/cgi-bin/setlink?base=preprint&amp;categ=CM-P&amp;id=CM-P00059253"/>
      <self-uri xlink:href="http://cds.cern.ch/record/955538/files/CM-P00059253.pdf"/>
      <self-uri xlink:href="http://cds.cern.ch/record/955538/files/04327300.pdf"/>
    </article-meta>
    <abstract>Two bunching schemes are considered in the frame of the CPS Linac, one with a single buncher, the other with a double-drift harmonic buncher. The matching of the beam to the Linac acceptance in six phase-space dimensions is achieved by computer programs in an iterative way: zero current solutions are found first, and then the intensity is progressively raised until 200 mA are trapped into the Linac. (9 refs) .</abstract>
  </front>
  <article-type>research-article</article-type>
  <ref/>
</article>

</articles>