Definition

Let GG be a acting by a on (M,ω)(M,\omega). With the convention ιXfω=df\iota_{X_f}\omega=df, the action is Hamiltonian if it admits a μ:Mg\mu:M\to\mathfrak g^* such that

dμ,ξ=ιξMωd\langle\mu,\xi\rangle=\iota_{\xi_M}\omega

for every ξg\xi\in\mathfrak g, and μ(gx)=Adgμ(x)\mu(gx)=\operatorname{Ad}_g^*\mu(x) for every gGg\in G. The triple (M,ω,μ)(M,\omega,\mu), together with the GG-action, is a Hamiltonian GG-space. Thus Hamiltonianity requires compatible global Hamiltonians for all infinitesimal generators, not merely preservation of ω\omega. Equivariance couples those Hamiltonians to the full .

Infinitesimal characterization

Symplecticity gives d(ιξMω)=0d(\iota_{\xi_M}\omega)=0. A moment map exists only if these closed one-forms are exact and their primitives can be chosen linearly in ξ\xi. Equivariance further requires

{μ,ξ,μ,η}=μ,[ξ,η]\{\langle\mu,\xi\rangle,\langle\mu,\eta\rangle\} =\langle\mu,[\xi,\eta]\rangle

with the compatible Poisson-bracket convention. For connected GG, 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 S1S^1 on R2\mathbb R^2 with ω=dxdy\omega=dx\wedge dy is Hamiltonian; a moment map is (x,y)(x2+y2)/2(x,y)\mapsto -(x^2+y^2)/2, after identifying s1\mathfrak{s}^1{}^* with R\mathbb R. 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
  1. Victor Guillemin and Shlomo Sternberg, Symplectic Techniques in Physics, Cambridge University Press, 1984. DOI record. Relevant: Chapter 3, Hamiltonian group actions and moment maps.
  2. Juan-Pablo Ortega and Tudor S. Ratiu, Momentum Maps and Hamiltonian Reduction, Birkhäuser, 2004. DOI record. Relevant: §4.2, momentum maps and equivariance.