Symplectomorphisms and Hamiltonian Diffeomorphisms
The group of symplectomorphisms of a symplectic manifold is the natural symmetry group in symplectic geometry. The subgroup of Hamiltonian diffeomorphisms plays a special role, as these are the symmetries generated by Hamiltonian flows.
Symplectomorphism Group
A symplectomorphism of is a diffeomorphism with . The group of all symplectomorphisms is denoted . Its Lie algebra consists of symplectic vector fields: with , equivalently .
A Hamiltonian diffeomorphism is the time-1 map of a (possibly time-dependent) Hamiltonian flow. The group of Hamiltonian diffeomorphisms is a normal subgroup of (the identity component). Its Lie algebra consists of Hamiltonian vector fields: where is exact.
The quotient is described by the flux homomorphism . A symplectomorphism is Hamiltonian if and only if it can be connected to the identity by a path with zero flux. When , every symplectomorphism isotopic to the identity is Hamiltonian.
Generating Functions
A symplectomorphism of close to the identity can be described by a generating function via the implicit equations , , where .
The fixed points of a Hamiltonian diffeomorphism correspond to critical points of an action functional. The Arnold conjecture predicts that . This lower bound by topology is a deep generalization of the PoincarΓ©-Birkhoff theorem and motivated the development of Floer homology.