Definition
Hamiltonian Lie group action
A symplectic Lie group action equipped with a compatible equivariant moment map.
Definition
Let be a Lie group acting by a symplectic Lie group action on . With the convention , the action is Hamiltonian if it admits a moment map such that
for every , and for every . The triple , together with the -action, is a Hamiltonian -space. Thus Hamiltonianity requires compatible global Hamiltonians for all infinitesimal generators, not merely preservation of . Equivariance couples those Hamiltonians to the full group action.
Infinitesimal characterization
Symplecticity gives . A moment map exists only if these closed one-forms are exact and their primitives can be chosen linearly in . Equivariance further requires
with the compatible Poisson-bracket convention. For connected , this infinitesimal bracket identity is equivalent to global coadjoint equivariance Ortega and Ratiu, §4.2.
Examples and non-examples
The standard counterclockwise rotation action of on with is Hamiltonian; a moment map is , after identifying with . Cotangent-lifted actions provide a canonical family of examples.
Translations on a symplectic torus preserve its symplectic form but need not be Hamiltonian: contraction with a generating translation field can be a closed nonexact one-form. The failed condition is global exactness, not symplecticity.
Conventions and scope
References
- Victor Guillemin and Shlomo Sternberg, Symplectic Techniques in Physics, Cambridge University Press, 1984. DOI record. Relevant: Chapter 3, Hamiltonian group actions and moment maps.
- Juan-Pablo Ortega and Tudor S. Ratiu, Momentum Maps and Hamiltonian Reduction, Birkhäuser, 2004. DOI record. Relevant: §4.2, momentum maps and equivariance.