<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Antipov, S. A.</author>
             <author>Nagaitsev, S.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Hénon-Heiles Single Particle Dynamics at IOTA
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-182-3</isbn>
		 <electronic-resource-num>10.18429/JACoW-IPAC2017-WEOAB1</electronic-resource-num>
		 <language>English</language>
		 <pages>2508-2511</pages>
       <pages>WEOAB1</pages>
       <keywords>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-05</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-IPAC2017-WEOAB1</url>
              <url>http://jacow.org/ipac2017/papers/weoab1.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          A Hénon-Heiles system is a simple, classical nonlinear Hamiltonian system offering a wide range of particle dynamics from regular orbits to resonant behavior to chaotic trajectories. Initially proposed to describe the motion of stars around a galactic center, it remains a vivid topic in Dynamics and Mathematical Physics since its discovery in 1964. Although the system and its modifications have been extensively studied numerically, its dynamics has never been observed in a controlled experiment. In this report we show that it is possible to create the Hénon-Heiles Hamiltonian using sextupoles in a realistic accelerator lattice. We propose a special sextupole channel to create the desired potential at the IOTA ring and study the 3D single particle dynamics by frequency map analysis and Poincare cross-sections. The proposed experiment would allow real world testing of regular and chaotic motion with a controlled strength of the nonlinearity.
       </abstract>
    </record>
  </records>
</xml>
