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＜電子ブック＞
Convexity Methods in Hamiltonian Mechanics / by Ivar Ekeland
(Ergebnisse der Mathematik und ihrer Grenzgebiete. 3. Folge / A Series of Modern Surveys in Mathematics. ISSN:21975655 ; 19)

版	1st ed. 1990.
出版者	(Berlin, Heidelberg : Springer Berlin Heidelberg : Imprint: Springer)
出版年	1990
本文言語	英語
大きさ	X, 247 p : online resource
著者標目	*Ekeland, Ivar author SpringerLink (Online service)
件　名	LCSH:Differential equations LCSH:Mathematical optimization LCSH:Calculus of variations LCSH:Mathematical physics LCSH:Game theory FREE:Differential Equations FREE:Calculus of Variations and Optimization FREE:Theoretical, Mathematical and Computational Physics FREE:Game Theory
一般注記	I. Linear Hamiltonian Systems -- 1. Floquet Theory and Stability -- 2. Krein Theory and Strong Stability -- 3. Time-Dependence of the Eigenvalues of R (t) -- 4. Index Theory for Positive Definite Systems -- 5. The Iteration Formula -- 6. The Index of a Periodic Solution to a Nonlinear Hamiltonian System -- 7. Examples -- 8. Non-periodic Solutions: The Mean Index -- II. Convex Hamiltonian Systems -- 1. Fundamentals of Convex Analysis -- 2. Convex Analysis on Banach Spaces -- 3. Integral Functionals on L? -- 4. The Clarke Duality Formula -- III. Fixed-Period Problems: The Sublinear Case -- 1. Subquadratic Hamiltonians -- 2. An Existence Result -- 3. Autonomous Systems -- 4. Nonautonomous Systems -- 5. Other Problems -- IV. Fixed-Period Problems: The Superlinear Case -- 1. Mountain-Pass Points -- 2. A Preliminary Existence Result -- 3. The Index at Mountain-Pass Points -- 4. Subharmonics -- 5. Autonomous Problems and Potential Wells -- V. Fixed-Energy Problems -- 1. Existence, Length, Stability -- 2. Multiplicity in the Pinched Case -- 3. Multiplicity in the General Case -- 4. Open Problems In the case of completely integrable systems, periodic solutions are found by inspection. For nonintegrable systems, such as the three-body problem in celestial mechanics, they are found by perturbation theory: there is a small parameter € in the problem, the mass of the perturbing body for instance, and for € = 0 the system becomes completely integrable. One then tries to show that its periodic solutions will subsist for € -# 0 small enough. Poincare also introduced global methods, relying on the topological properties of the flow, and the fact that it preserves the 2-form L~=l dPi 1\ dqi' The most celebrated result he obtained in this direction is his last geometric theorem, which states that an area-preserving map of the annulus which rotates the inner circle and the outer circle in opposite directions must have two fixed points. And now another ancient theme appear: the least action principle. It states that the periodic solutions of a Hamiltonian system are extremals of a suitable integral over closed curves. In other words, the problem is variational. This fact was known to Fermat, and Maupertuis put it in the Hamiltonian formalism. In spite of its great aesthetic appeal, the least action principle has had little impact in Hamiltonian mechanics. There is, of course, one exception, Emmy Noether's theorem, which relates integrals ofthe motion to symmetries of the equations. But until recently, no periodic solution had ever been found by variational methods HTTP:URL=https://doi.org/10.1007/978-3-642-74331-3

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