Let GG be a with a on (M,ω)(M,\omega), and let g\mathfrak g be its . Write g=HomR(g,R)\mathfrak g^*=\operatorname{Hom}_{\mathbb R}(\mathfrak g,\mathbb R) for its linear dual.

For ξg\xi\in\mathfrak g, use the fundamental vector field ξM(x)=ddtt=0exp(tξ)x\xi_M(x)=\left.\frac{d}{dt}\right|_{t=0}\exp(t\xi)\cdot x, where exp\exp is the .

A moment map for the action is a

μ ⁣:Mg\mu\colon M \to \mathfrak{g}^*

such that for every ξg\xi\in\mathfrak{g},

dμ,ξ  =  ιξMω,d\langle \mu,\xi\rangle \;=\; \iota_{\xi_M}\omega,

where dd is the and ιξM\iota_{\xi_M} denotes by the vector field ξM\xi_M.

Conventions and uniqueness

This definition does not impose equivariance. An equivariant moment map also satisfies μ(gx)=Adgμ(x)\mu(gx)=\operatorname{Ad}_g^*\mu(x) for the . The entry uses this stronger convention; some authors call an action Hamiltonian as soon as it has a moment map in the present sense. A different sign convention may replace the displayed identity by its negative.

If MM is connected, any two moment maps satisfying the displayed identity differ by a constant in g\mathfrak{g}^*. If both are equivariant, that constant is fixed by the coadjoint action.

For an equivariant moment map, a useful reformulation is that in (Cartan model), the pair (ω,μ)(\omega,\mu) combines into an equivariantly closed degree-2 element.

Examples
  1. Rotation of the plane. For the standard counterclockwise S1S^1-action on R2C\mathbb{R}^2\cong \mathbb{C}, the unsigned left-action generator, and ω=dxdy\omega=dx\wedge dy, a moment map is μ(z)=12z2\mu(z)=-\tfrac12|z|^2 (identifying (u(1))R(\mathfrak{u}(1))^*\cong \mathbb{R}).
  2. Height on the 2-sphere. For the standard rotation action of S1S^1 on S2S^2 around the vertical axis with the area form, a moment map is the height function (up to an additive constant).
  3. . If GG acts on a manifold QQ, the induced action on TQT^*Q with its canonical symplectic form is Hamiltonian, with moment map μ(q,p)(ξ)=p(ξQ(q))\mu(q,p)(\xi)=p(\xi_Q(q)).