Definition

Let a GG act symplectically on (M,ω)(M,\omega), and let μ:Mg\mu:M\to\mathfrak g^* be a . It is an equivariant moment map if

μ(gx)=Adgμ(x)\mu(g\cdot x)=\operatorname{Ad}_g^*\mu(x)

for every gGg\in G and xMx\in M, where Ad\operatorname{Ad}^* is the . Thus μ\mu satisfies both the differential moment-map identity for every ξg\xi\in\mathfrak g and the global compatibility condition intertwining the two GG-actions.

Infinitesimal criterion

Differentiating equivariance at the identity gives

dμx(ξM(x))=adξμ(x).d\mu_x\bigl(\xi_M(x)\bigr)=\operatorname{ad}_\xi^*\mu(x).

With the coadjoint convention Adgλ=λAdg1\operatorname{Ad}_g^*\lambda=\lambda\circ\operatorname{Ad}_{g^{-1}}, this formula uses the corresponding infinitesimal coadjoint action. If GG is connected, the infinitesimal identity for every ξ\xi implies the global equivariance condition Ortega and Ratiu, §4.2.

Equivariance defect

For a nonequivariant moment map, the difference

σ(g)=μ(gx)Adgμ(x)\sigma(g)=\mu(g\cdot x)-\operatorname{Ad}_g^*\mu(x)

is independent of xx when MM is connected and defines a group cocycle with values in g\mathfrak g^*. Changing μ\mu by a constant changes this cocycle by a coboundary. Consequently, the obstruction to choosing an equivariant moment map is a cohomology class rather than merely a poor normalization.

Consequences and conventions

Equivariance makes inverse images of coadjoint-invariant subsets GG-invariant and is the hypothesis normally used in Hamiltonian reduction. Sign conventions for the , the moment-map equation, and the infinitesimal coadjoint action vary together in the literature; the global equation in the core is convention-independent once the cited coadjoint action has been fixed.

References
  1. J.-P. Ortega and T. S. Ratiu, Momentum Maps and Hamiltonian Reduction, Birkhäuser, 2004. Springer DOI record. Relevant: §4.2.
  2. V. Guillemin and S. Sternberg, Symplectic Techniques in Physics, Cambridge University Press, 1990. Cambridge DOI record. Relevant: Chapter 3.