<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Hart, T.L.</author>
             <author>Acosta, J.G.</author>
             <author>Cremaldi, L.M.</author>
             <author>Neuffer, D.V.</author>
             <author>Oliveros, S.J.</author>
             <author>Summers, D.J.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Final 6d Muon Ionization Cooling Using Strong Focusing Quadrupoles
          </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-TUPOB44</electronic-resource-num>
		 <language>English</language>
		 <pages>592-595</pages>
       <pages>TUPOB44</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>emittance</keyword>
          <keyword>quadrupole</keyword>
          <keyword>betatron</keyword>
          <keyword>collider</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-TUPOB44</url>
              <url>https://jacow.org/napac2016/papers/tupob44.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          Low emittance muon beam lines and muon colliders are potentially a rich source of BSM physics for future experimenters. A normalized transverse muon emittance of 280 microns has been achieved in simulation with short solenoids and a betatron function of 3 cm. Here we use ICOOL, G4Beamline, and MAD-X to explore using a flat 400 MeV/c muon beam and strong focusing quadrupoles to achieve a normalized transverse emittance of 100 microns and finish 6D cooling. The low beta regions, as low as 5 mm, produced by the quadrupoles are occupied by dense, low Z absorbers, such as lithium hydride or beryllium, that cool the beam. Equilibrium transverse emittance is linearly proportional to the beta function. Reverse emittance exchange with septa and/or wedges is then used to decrease transverse emittance from 100 to 25 microns at the expense of longitudinal emittance for a high energy lepton collider. Cooling challenges include chromaticity correction, momentum passband overlap, quadrupole acceptance, and staying in phase with RF.
       </abstract>
    </record>
  </records>
</xml>
