Definition

Let GG act on a (M,ω)(M,\omega), let μ:Mg\mu:M\to\mathfrak g^* be a , and fix ξg\xi\in\mathfrak g. The moment-map component in the direction ξ\xi is the smooth function

μξ:MR,μξ(p)=μ(p),ξ.\mu^\xi:M\to\mathbb R,\qquad \mu^\xi(p)=\langle\mu(p),\xi\rangle.

With the conventions

ξM(p)=ddt0exp(tξ)p,dμξ=ιξMω,\xi_M(p)=\left.\frac{d}{dt}\right|_0\exp(t\xi)\mathbin{\cdot}p, \qquad d\mu^\xi=\iota_{\xi_M}\omega,

the function μξ\mu^\xi is a for the ξM\xi_M. It records the Hamiltonian associated with one infinitesimal symmetry.

Linearity and reconstruction

The assignment ξμξ\xi\mapsto\mu^\xi is linear from g\mathfrak g to C(M)C^\infty(M). Conversely, a linear family of functions HξH_\xi determines a map μ:Mg\mu:M\to\mathfrak g^* by μ(p),ξ=Hξ(p)\langle\mu(p),\xi\rangle=H_\xi(p). Thus the component equations for all ξ\xi are equivalent to the single g\mathfrak g^*-valued moment-map equation.

Equivariance and constants

If μ\mu is equivariant for the , then

μξ(gp)=μAdg1ξ(p).\mu^\xi(g\mathbin{\cdot}p)=\mu^{\operatorname{Ad}_{g^{-1}}\xi}(p).

Adding a constant cgc\in\mathfrak g^* shifts each component by c,ξ\langle c,\xi\rangle without changing its differential. Equivariance is preserved precisely when cc is fixed by the coadjoint action.

Examples and conventions

For the on TQT^*Q, the standard component is μξ(q,α)=α(ξQ(q))\mu^\xi(q,\alpha)=\alpha(\xi_Q(q)). On a with its , the inclusion moment map has μξ(λ)=λ,ξ\mu^\xi(\lambda)=\langle\lambda,\xi\rangle. Authors using dμξ=ιξMωd\mu^\xi=-\iota_{\xi_M}\omega obtain the negative components relative to the present convention.

References
  1. Juan-Pablo Ortega and Tudor S. Ratiu, Momentum Maps and Hamiltonian Reduction, Progress in Mathematics 222, Birkhäuser, 2004. DOI record. Relevant: Chapter 4, the standard momentum map and its component functions.
  2. Ana Cannas da Silva, Lectures on Symplectic Geometry, Lecture Notes in Mathematics 1764, Springer, 2001. DOI record. Relevant: Chapter 5, Hamiltonian actions and moment maps.