nLab
Poisson manifold

Contents

Idea

Poisson manifolds are a mathematical setup for classical mechanics with finitely many degrees of freedom.

Definition

A Poisson algebra is a commutative unital associative algebra A, in this case over the field of real or complex numbers, equipped with a Lie bracket {,}:AAA such that, for any fA, {f,}:AA is a derivation of A as an associative algebra.

A Poisson manifold is a real smooth manifold M equipped with a Poisson structure. A Poisson structure is a Lie algebra bracket {,}:C (M)×C (M)C (M) on the vector space of smooth functions on M which together with the pointwise multiplication of functions makes it a Poisson algebra. As derivations of C (M) correspond to smooth tangent vector fields, for each fC (M) there is a vector X f given by X f(g)={f,g} and called the Hamiltonian vector field corresponding to the function f, which is viewed as a classical hamiltonian function.

Alternatively a Poisson structure on a manifold is given by a choice of smooth antisymmetric bivector called a Poisson bivector PΛ 2TM; then {f,g}:=dfdg,P.

This induces and is equivalently encoded by the structure of a Poisson Lie algebroid.

A morphism h:MN of Poisson manifolds is a morphism of smooth manifolds such that, for all f,gC (N), {fh,gh} M={f,g} N.

Examples

Every symplectic manifold carries a natural Poisson structure; however, such Poisson manifolds are very special. It is a basic theorem that Poisson structures on a manifold are equivalent to the smooth foliations of the underlying manifold such that each leaf is a symplectic manifold.

The dual to a finite-dimensional Lie algebra has a natural structure of a Poisson manifold due to Kirillov. Its leaves are called coadjoint orbits.

Properties

Kontsevich formality implies that every Poisson manifold has a canonical deformation quantization.