<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Neuffer, D.V.</author>
             <author>Hart, T.L.</author>
             <author>Sayed, H. K.</author>
             <author>Summers, D.J.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Final Cooling For a High-luminosity High-energy Lepton Collider
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-168-7</isbn>
		 <electronic-resource-num>10.18429/JACoW-IPAC2015-TUBD2</electronic-resource-num>
		 <language>English</language>
		 <pages>1384-1386</pages>
       <pages>TUBD2</pages>
       <keywords>
          <keyword>emittance</keyword>
          <keyword>collider</keyword>
          <keyword>luminosity</keyword>
          <keyword>solenoid</keyword>
          <keyword>linac</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2015</year>
          <pub-dates>
             <date>2015-06</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-IPAC2015-TUBD2</url>
              <url>http://jacow.org/ipac2015/papers/tubd2.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The final cooling system for a high-energy high-luminosity muon collider requires reduction of the transverse emittance by an order of magnitude to ~0.00003 m (rms, N), while allowing longitudinal emittance increase to ~0.1m. In the present baseline approach, this is obtained by transverse cooling of low-energy muons within a sequence of high field solenoids with low-frequency rf systems. Recent studies of such systems are presented. Since the final cooling steps are actually emittance exchange a variant form of that final system can be obtained by a round to flat transform in x-y, with transverse slicing of the enlarged flat transverse dimension followed by longitudinal recombination of the sliced bunchlets. Development of final exchange following lowest-emittance cooling is discussed.
       </abstract>
    </record>
  </records>
</xml>
