ConceptComplete

Moment Maps

The moment map is a fundamental tool linking Hamiltonian group actions on symplectic manifolds to the dual of the Lie algebra. It generalizes classical conserved quantities (linear and angular momentum) to arbitrary symmetry groups.


Definition and Properties

Definition5.1Moment Map

Let (M,ω)(M, \omega) be a symplectic manifold with a Hamiltonian action of a Lie group GG. A moment map is a smooth map μ:Mg\mu: M \to \mathfrak{g}^* satisfying:

  1. For each ξg\xi \in \mathfrak{g}, the function μξ=μ,ξ:MR\mu_\xi = \langle \mu, \xi \rangle: M \to \mathbb{R} is a Hamiltonian for the infinitesimal generator XξX_\xi: dμξ=ιXξωd\mu_\xi = \iota_{X_\xi}\omega.
  2. Equivariance: μ(gx)=Adgμ(x)\mu(g \cdot x) = \mathrm{Ad}_g^* \cdot \mu(x) for all gG,xMg \in G, x \in M.
Definition5.2Comoment Map

The comoment map μ~:gC(M)\tilde{\mu}: \mathfrak{g} \to C^\infty(M) is defined by μ~(ξ)=μξ\tilde{\mu}(\xi) = \mu_\xi. The equivariance of μ\mu is equivalent to μ~\tilde{\mu} being a Lie algebra homomorphism: μ~([ξ,η])={μ~(ξ),μ~(η)}\tilde{\mu}([\xi, \eta]) = \{\tilde{\mu}(\xi), \tilde{\mu}(\eta)\}.

ExampleMoment Map on $T^*G$

The left GG-action on TGT^*G by cotangent lifts is Hamiltonian with moment map μL:TGg\mu_L: T^*G \to \mathfrak{g}^* given by μL(αg)=(dRg)αg\mu_L(\alpha_g) = (dR_g)^* \alpha_g (right-trivialization). This identifies TGT^*G with G×gG \times \mathfrak{g}^*.


Existence and Uniqueness

RemarkObstructions to Existence

A moment map exists if and only if the action is Hamiltonian, which requires the infinitesimal generators to be Hamiltonian vector fields. The obstruction lies in H1(M;R)H^1(M; \mathbb{R}) (whether ιXξω\iota_{X_\xi}\omega is exact) and in H2(g;R)H^2(\mathfrak{g}; \mathbb{R}) (whether the comoment map can be made a Lie algebra homomorphism). When both vanish, μ\mu exists and is unique up to a constant in (g)G(\mathfrak{g}^*)^G.

Definition5.3Hamiltonian $G$-Space

A Hamiltonian GG-space is a triple (M,ω,μ)(M, \omega, \mu) where (M,ω)(M, \omega) is a symplectic manifold, GG acts on MM preserving ω\omega, and μ:Mg\mu: M \to \mathfrak{g}^* is an equivariant moment map. This is the standard setup for symplectic reduction and geometric quantization.