Download The Geometry of Hamiltonian Systems: Proceedings of a by Malcolm R. Adams, Maarten Bergvelt (auth.), Tudor Ratiu PDF

By Malcolm R. Adams, Maarten Bergvelt (auth.), Tudor Ratiu (eds.)

The papers during this quantity are an outgrowth of the lectures and casual discussions that came about through the workshop on "The Geometry of Hamiltonian platforms" which used to be held at MSRl from June five to sixteen, 1989. It used to be, in a few feel, the final significant occasion of the year-long software on Symplectic Geometry and Mechanics. The emphasis of the entire talks was once on Hamiltonian dynamics and its courting to a number of elements of symplectic geometry and topology, mechanics, and dynamical structures more often than not. The organizers of the convention have been R. Devaney (co-chairman), H. Flaschka (co-chairman), okay. Meyer, and T. Ratiu. the complete assembly used to be equipped round mini-courses of 5 lectures every one and a sequence of 2 expository lectures. the 1st of the mini-courses was once given by means of A. T. Fomenko, who provided the paintings of his staff at Moscow college at the type of integrable structures. the second one mini­ direction was once given via J. Marsden of UC Berkeley, who spoke approximately numerous purposes of symplectic and Poisson aid to difficulties in balance, basic kinds, and symmetric Hamiltonian bifurcation concept. eventually, the 2 expository talks got by means of A. Fathi of the college of Florida who focused on the hyperlinks among symplectic geometry, dynamical platforms, and Teichmiiller theory.

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Extra resources for The Geometry of Hamiltonian Systems: Proceedings of a Workshop Held June 5–16, 1989

Example text

The corresponding reduced Poisson algebra is (WOO(MI')' { ,} ). I' It follows from the definitions that the underlying function space can be represented as WOO (MI') = COO(MjG)jI(MI') COO(M)G jI(J- 1 (OI'))G COO(M)G jI(J-l(p,))G where I(J-l(p,))G is the ideal of smooth G-inyariant functions on M which vanish on J-l(p,). In the last equality we have used the fact that J- 1 (OI') = G· J- 1 (p,), which is a consequence of the Ad--equivariance of J. Formally we see that reduction in singular cases works exactly as it does in regular cases.

1160, Springer Verlag, New York, 1985. 10. , On resonant Hamiltonian systems with finitely many degrees of freedom, Lect. , 252, (1986), 19-31. 11. , Realizations of the reduced phase space of a Hamiltonian system with symmetry, Lect. , 252, (1986), 32-39. 12. , Spaces of solutions of relativistic field theories with constraints, Lect. , 987, (1982), 29-43. 13. , Symmetry and solution set singularities in Hamiltonian field theories, Acta Phys. , B17, (1986), 499-523 14. , Poisson reduction and quantization for the (n+l)-photon, J.

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