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180421s2018 riu o 000 0 eng d |
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|a 2018005046
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|a EBLCP
|b eng
|e pn
|c EBLCP
|d OCLCQ
|d IDB
|d OCLCF
|d OCLCQ
|d K6U
|d S9M
|d GZM
|d UIU
|d CUY
|d COD
|d YDX
|d COO
|d LEAUB
|d UKAHL
|d VLY
|d VT2
|d OCLCO
|d OCLCQ
|d OCLCO
|d S9M
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|a 1028580070
|a 1159411994
|a 1262687483
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|a 9781470443733
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|a 1470443732
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|a 1470428016
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|a 9781470428013
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|a (OCoLC)1031968034
|z (OCoLC)1028580070
|z (OCoLC)1159411994
|z (OCoLC)1262687483
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|a QC20.7.H35
|b .P385 2018eb
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|a HCDD
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|a Paulo, Naiara V. de,
|d 1986-
|1 https://id.oclc.org/worldcat/entity/E39PCjGqWVQvMCXTdxyvmqYqXq
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|a Systems of Transversal Sections near Critical Energy Levels of Hamiltonian Systems in R⁴
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|a Providence :
|b American Mathematical Society,
|c 2018.
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|a 1 online resource (118 pages)
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|a text
|b txt
|2 rdacontent
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|a computer
|b c
|2 rdamedia
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|a online resource
|b cr
|2 rdacarrier
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|a Memoirs of the American Mathematical Society Ser. ;
|v v. 252
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|a Print version record.
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|a 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).
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|a Appendix A. Basics on pseudo-holomorphic curves in symplectizationsAppendix B. Linking properties; Appendix C. Uniqueness and intersections of pseudo-holomorphic curves; References; Back Cover.
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|a 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 \mathc.
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|a Includes bibliographical references (pages 103-105).
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|a Hamiltonian systems.
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|a Energy levels (Quantum mechanics)
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|a Vector fields.
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|a Campos vectoriales
|2 embne
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|a Sistemas de Hamilton
|2 embne
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|a Energy levels (Quantum mechanics)
|2 fast
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|a Hamiltonian systems
|2 fast
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|a Vector fields
|2 fast
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|a Salomão, Pedro A. S.
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|i has work:
|a Systems of Transversal Sections near Critical Energy Levels of Hamiltonian Systems in R⁴ (Text)
|1 https://id.oclc.org/worldcat/entity/E39PCFH3MGdt3fJxp49CHRRxQm
|4 https://id.oclc.org/worldcat/ontology/hasWork
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776 |
0 |
8 |
|i Print version:
|a De, Naiara V.
|t Systems of Transversal Sections near Critical Energy Levels of Hamiltonian Systems in R⁴.
|d Providence : American Mathematical Society, ©2018
|z 9781470428013
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830 |
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0 |
|a Memoirs of the American Mathematical Society Ser.
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856 |
4 |
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|u https://ebookcentral.proquest.com/lib/holycrosscollege-ebooks/detail.action?docID=5347056
|y Click for online access
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903 |
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|a EBC-AC
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994 |
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|a 92
|b HCD
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