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Systems of Transversal Sections near Critical Energy Levels of Hamiltonian Systems in

By: Contributor(s): Material type: TextTextSeries: Memoirs of the American Mathematical Society SeriesPublisher: Providence : American Mathematical Society, 2018Copyright date: ©2018Edition: 1st edDescription: 1 online resource (118 pages)Content type:
  • text
Media type:
  • computer
Carrier type:
  • online resource
ISBN:
  • 9781470443733
Subject(s): Genre/Form: Additional physical formats: Print version:: Systems of Transversal Sections near Critical Energy Levels of Hamiltonian Systems in DDC classification:
  • 514/.74
LOC classification:
  • QC20.7.H35 .P385 2018
Online resources:
Contents:
Cover -- Title page -- Chapter 1. Introduction -- 1.1. Saddle-center equilibrium points -- 1.2. Strictly convex subsets of the critical energy level -- 1.3. 2-3 foliations -- 1.4. Main statement -- 1.5. Applications -- 1.6. An open question -- Chapter 2. Proof of the main statement -- Chapter 3. Proof of Proposition 2.1 -- Chapter 4. Proof of Proposition 2.2 -- Chapter 5. Proof of Proposition 2.8 -- Chapter 6. Proof of Proposition 2.9 -- Chapter 7. Proof of Proposition 2.10- ) -- Chapter 8. Proof of Proposition 2.10-ii) -- Chapter 9. Proof of Proposition 2.10-iii) -- Appendix A. Basics on pseudo-holomorphic curves in symplectizations -- Appendix B. Linking properties -- Appendix C. Uniqueness and intersections of pseudo-holomorphic curves -- References -- Back Cover.
Summary: In this article the authors study Hamiltonian flows associated to smooth functions H:\mathbb R^4 \to \mathbb R restricted to energy levels close to critical levels. They assume the existence of a saddle-center equilibrium point p_c in the zero energy level H^{-1}(0). The Hamiltonian function near p_c is assumed to satisfy Moser's normal form and p_c is assumed to lie in a strictly convex singular subset S_0 of H^{-1}(0). Then for all E \gt 0 small, the energy level H^{-1}(E) contains a subset S_E near S_0, diffeomorphic to the closed 3-ball, which admits a system of transversal sections \mathcal F_E, called a 2-3 foliation. \mathcal F_E is a singular foliation of S_E and contains two periodic orbits P_2,E\subset \partial S_E and P_3,E\subset S_E\setminus \partial S_E as binding orbits. P_2,E is the Lyapunoff orbit lying in the center manifold of p_c, has Conley-Zehnder index 2 and spans two rigid planes in \partial S_E. P_3,E has Conley-Zehnder index 3 and spans a one parameter family of planes in S_E \setminus \partial S_E. A rigid cylinder connecting P_3,E to P_2,E completes \mathcal F_E. All regular leaves are transverse to the Hamiltonian vector field. The existence of a homoclinic orbit to P_2,E in S_E\setminus \partial S_E follows from this foliation.
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Cover -- Title page -- Chapter 1. Introduction -- 1.1. Saddle-center equilibrium points -- 1.2. Strictly convex subsets of the critical energy level -- 1.3. 2-3 foliations -- 1.4. Main statement -- 1.5. Applications -- 1.6. An open question -- Chapter 2. Proof of the main statement -- Chapter 3. Proof of Proposition 2.1 -- Chapter 4. Proof of Proposition 2.2 -- Chapter 5. Proof of Proposition 2.8 -- Chapter 6. Proof of Proposition 2.9 -- Chapter 7. Proof of Proposition 2.10- ) -- Chapter 8. Proof of Proposition 2.10-ii) -- Chapter 9. Proof of Proposition 2.10-iii) -- Appendix A. Basics on pseudo-holomorphic curves in symplectizations -- Appendix B. Linking properties -- Appendix C. Uniqueness and intersections of pseudo-holomorphic curves -- References -- Back Cover.

In this article the authors study Hamiltonian flows associated to smooth functions H:\mathbb R^4 \to \mathbb R restricted to energy levels close to critical levels. They assume the existence of a saddle-center equilibrium point p_c in the zero energy level H^{-1}(0). The Hamiltonian function near p_c is assumed to satisfy Moser's normal form and p_c is assumed to lie in a strictly convex singular subset S_0 of H^{-1}(0). Then for all E \gt 0 small, the energy level H^{-1}(E) contains a subset S_E near S_0, diffeomorphic to the closed 3-ball, which admits a system of transversal sections \mathcal F_E, called a 2-3 foliation. \mathcal F_E is a singular foliation of S_E and contains two periodic orbits P_2,E\subset \partial S_E and P_3,E\subset S_E\setminus \partial S_E as binding orbits. P_2,E is the Lyapunoff orbit lying in the center manifold of p_c, has Conley-Zehnder index 2 and spans two rigid planes in \partial S_E. P_3,E has Conley-Zehnder index 3 and spans a one parameter family of planes in S_E \setminus \partial S_E. A rigid cylinder connecting P_3,E to P_2,E completes \mathcal F_E. All regular leaves are transverse to the Hamiltonian vector field. The existence of a homoclinic orbit to P_2,E in S_E\setminus \partial S_E follows from this foliation.

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Electronic reproduction. Ann Arbor, Michigan : ProQuest Ebook Central, 2024. Available via World Wide Web. Access may be limited to ProQuest Ebook Central affiliated libraries.

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