Definition
Comoment map
A Lie algebra homomorphism assigning to each infinitesimal symmetry its Hamiltonian function.
Definition
Let act on by a symplectic action, with Lie algebra , and use . A comoment map is a linear map
such that and
for all . Thus is a Lie algebra homomorphism into the Poisson algebra of smooth functions, and each generates the infinitesimal action associated with . The differential axiom identifies the generating vector fields; the bracket axiom requires the chosen Hamiltonians to respect the Lie algebra exactly, rather than only up to constants.
Relationship to moment maps
A moment map determines the linear assignment
The differential condition for is exactly the componentwise moment-map identity. Under the conventions in the core, the bracket condition is infinitesimal equivariance of ; for connected , it is equivalent to global coadjoint equivariance Ortega and Ratiu, §4.2.
Conversely, a comoment map defines uniquely by , because is linear in .
Obstruction to bracket preservation
If a linear choice of Hamiltonians satisfies only the differential condition, then
is locally constant on . On a connected manifold it is a real-valued Lie-algebra -cocycle. Changing by constants changes by a coboundary, so the resulting cohomology class measures the obstruction to converting the weak assignment into a comoment map.
Conventions and scope
References
- Victor Guillemin and Shlomo Sternberg, Symplectic Techniques in Physics, Cambridge University Press, 1984. DOI record. Relevant: Chapter 3, infinitesimal Hamiltonians and moment maps.
- Juan-Pablo Ortega and Tudor S. Ratiu, Momentum Maps and Hamiltonian Reduction, Birkhäuser, 2004. DOI record. Relevant: §4.2, infinitesimal equivariance and the cocycle obstruction.