A moment map is a dual incarnation of a Hamiltonian action of a Lie group (or Lie algebra) on a symplectic manifold.
An action of a Lie group $G$ on a symplectic manifold $X$ by (Hamiltonian) symplectomorphisms corresponds infinitesimally to a Lie algebra homomorphism from the Lie algebra $\mathfrak{g}$ to the Hamiltonian vector fields on $X$. If this lifts to a coherent choice of Hamiltonians, hence to a Lie algebra homomorphism $\mathfrak{g} \to (C^\infty(X), \{-,-\})$ to the Poisson bracket, then, by dualization, this is equivalently a Poisson manifold homomorphism of the form
This $\mu$ is called the moment map or momentum map of the Hamiltonian action.
The name derives from the special and historically first case of angular momentum in the dynamics of rigid bodies, see Examples - Angular momentum below.
The Preliminaries below review some basics of Hamiltonian vector fields. The definition of the moment map itself is below in Hamiltonian action and the moment map.
This section briefly reviews the notion of Hamiltonian vector fields on a symplectic manifold
The basic setup is the following: Let $(M,\omega)$ be a symplectic manifold with a Hamiltonian action of a Lie group $G$. In particular that means that there is an action $\nu\colon G \times M \to M$ via symplectomorphisms (diffeomorphisms $\nu_g$ such that $\nu_g^*(\omega) = \omega$). A vector field $X$ is symplectic if the corresponding flow preserves (again by pullbacks) $\omega$. The symplectic vector fields form a Lie subalgebra $\chi(M,\omega)$ of the Lie algebra of all smooth vector fields $\chi(M)$ on $M$ with respect to the Lie bracket.
By the Cartan homotopy formula and closedness $d \omega = 0$
where $\mathcal{L}_X$ denotes the Lie derivative. Therefore a vector field $X$ is symplectic iff $\iota(X)\omega = d H$ for some function $H\in C^\infty(M)$, usually called Hamiltonian (function) for $X$. Here $X$ is determined by $H$ up to a locally constant function. Such $X = X_H$ is called the Hamiltonian vector field corresponding to $H$. The Poisson structure on $M$ is the bracket $\{,\}$ on functions may be given by
where there is a Lie bracket of vector fields on the right hand side.
For $(M,\omega)$ a connected symplectic manifold, there is an exact sequence of Lie algebras
See at Hamiltonian vector field – Relation to Poisson bracket.
Let $(X, \omega)$ be a symplectic manifold and let $\mathfrak{g}$ be a Lie algebra. Write $(C^\infty(X), \{-,-\})$ for the Poisson bracket Lie algebra underlying the corresponding Poisson algebra.
A Hamiltonian action of $\mathfrak{g}$ on $(X, \omega)$ is a Lie algebra homomorphism
The corresponding function
to the dual vector space of $\mathfrak{g}$, defined by
is the corresponding moment map.
If one writes the evaluation pairing as
then the equation characterizing $\mu$ in def. reads for all $x \in X$ and $v \in \mathfrak{g}$
This is the way it is often written in the literature.
Notice that this in turn means that
The following are equivalent
the linear map underlying $\tilde\mu$ in def. is Lie algebra homomorphism;
its dual $\mu$ is a Poisson manifold homomorphism with respect to the Lie-Poisson structure on $\mathfrak{g}^\ast$.
This follows by just unwinding the definitions.
In one direction, suppose that $\tilde \mu$ is a Lie homomorphism. Since the Lie-Poisson structure is fixed on linear functions on $\mathfrak{g}^\ast$, it is sufficient to check that $\mu^\ast$ preserves the Poisson bracket on these. Consider hence two Lie algebra elements $v_1, v_2 \in \mathfrak{g}$ regarded as linear functions $\langle -,v_i\rangle$ on $\mathfrak{g}^\ast$. Noticing that on such linear functions the Lie-Poisson structure is given by the Lie bracket we have, using remark
and hence $\mu^\ast$ preserves the Poisson brackets.
Conversely, suppose that $\mu$ is a Poisson homomorphism. Then
and so $\tilde \mu$ is a Lie homomorphism.
Consider the action of SO(3) on $\mathbb{R}^3$, which induces a Hamiltonian action on $T^*\mathbb{R}^3\cong\mathbb{R}^3\times\mathbb{R}^3$ via
where $q$ is a column vector and $p$ is a row vector. Then the moment map for this Hamiltonian action is
where
If we choose $\Omega_1,\Omega_2,\Omega_3$ as an orthonormal basis of $\mathfrak{so}(3)$ and then identify $\mathfrak{so}(3)\cong\mathfrak{so}(3)^*\cong\mathbb{R}^3$, then $\mu(q,p)=\vec q\times\vec p$, which is the angular momentum.
The values of the moment map for each given Lie algebra generator may be regarded as the conserved currents given by a Hamiltonian Noether theorem.
Specifically if $(X,\omega)$ is a symplectic manifold equipped with a “time evolution” Hamiltonian action $\mathbb{R} \to \mathfrak{Poisson}(X,\omega)$ given by a Hamiltonian $H$ and if $\mathfrak{g} \to \mathfrak{Poisson}(X,\omega)$ is some Hamiltonian action with moment $\Phi(\xi)$ for $\xi \in \mathfrak{g}$ which preserves the Hamiltonian in that the Poisson bracket vanishes
then of course also the time evolution of the moments vanishes
See at Noether theorem – In terms of moment maps/Hamiltonian Noether theorem.
In the context of constrained mechanics? the components of the moment map (as the Lie algebra argument varies) are called first class constraints. See symplectic reduction for more.
The moment map is a crucial ingredient in the construction of Marsden–Weinstein symplectic quotients and in other variants of symplectic reduction.
The concept is originally due to Jean-Marie Souriau.
Lecture notes and surveys include
Joel W. Robbin, The moment map, an exposition, pdf
Nicole Berline, Michèle Vergne, Hamiltonian manifolds and moment maps (pdf)
Original articles include
Victor Guillemin, Shlomo Sternberg, Geometric asymptotics, AMS (1977) (online)
Michael Atiyah, Convexity and commuting Hamiltonians, Bull. London
Math. Soc. 14 (1982), 1-15.
Michael Atiyah, Raoul Bott, The moment map and equivariant cohomology, Topology, Vol 23, No. 1 (1984) (pdf)
Further developments are in
M. Spera, On a generalized uncertainty principle, coherent states and the moment map, J. of Geometry and Physics 12 (1993) 165-182, MR94m:58097, doi
Ctirad Klimcik, Pavol Severa, T-duality and the moment map, IHES/P/96/70, hep-th/9610198; Poisson-Lie T-duality: open strings and D-branes, CERN-TH/95-339. Phys.Lett. B376 (1996) 82-89, hep-th/9512124
A. Cannas da Silva, Alan Weinstein, Geometric models for noncommutative algebras, Berkeley Math. Lec. Notes Series, AMS 1999, (pdf)
Friedrich Knop, Automorphisms of multiplicity free Hamiltonian manifolds, arxiv/1002.4256
W. Crawley-Boevey, Geometry of the moment map for representations of quivers, Compositio Math. 126 (2001), no. 3, 257-293.
See also
Moment maps in higher geometry, Higher geometric prequantum theory, are discussed in
Reviews include for instance
Relation to equivariant cohomology:
Anton Alekseev, Anton Malkin, Eckhard Meinrenken, Lie group valued moment maps, J. Differential Geom. Volume 48, Number 3 (1998), 445-495. euclid, MR1638045
Eckhard Meinrenken, Lectures on group-valued moment maps and Verlinde formulas, 35 pages, January 2012, pdf
The relation between moment maps and conserved currents/Noether's theorem is amplied for instance in
Since moment maps generalize energy-functionals, they provide a covariant formulation of thermodynamics:
Jean-Marie Souriau, Thermodynamique et géométrie, Lecture Notes in Math. 676 (1978), 369–397 (scan)
Patrick Iglesias-Zemmour, Jean-Marie Souriau Heat, cold and Geometry, in: M. Cahen et al (eds.) Differential geometry and mathematical physics, 37-68, D. Reidel 1983 (web, pdf, doi:978-94-009-7022-9_5)
Jean-Marie Souriau, chapter IV “Statistical mechanics” of Structure of dynamical systems. A symplectic view of physics . Translated from the French by C. H. Cushman-de Vries. Translation edited and with a preface by R. H. Cushman and G. M. Tuynman. Progress in Mathematics, 149. Birkhäuser Boston, Inc., Boston, MA, 1997
Patrick Iglesias-Zemmour, Essai de «thermodynamique rationnelle» des milieux continus, Annales de l’I.H.P. Physique théorique, Volume 34 (1981) no. 1, p. 1-24 (numdam:AIHPA_1981__34_1_1_0)
Review includes
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