Definition

Let (M,{,}M)(M,\{-,-\}_M) and (N,{,}N)(N,\{-,-\}_N) be . A Φ:MN\Phi:M\to N is a Poisson map if

{f,g}NΦ={fΦ,gΦ}M\{f,g\}_N\circ\Phi=\{f\circ\Phi,g\circ\Phi\}_M

for all f,gC(N)f,g\in C^\infty(N). Thus the pullback homomorphism Φ:C(N)C(M)\Phi^*:C^\infty(N)\to C^\infty(M) is also a homomorphism of Poisson algebras. If πM\pi_M and πN\pi_N are the corresponding Poisson bivectors, the same condition is

(2dΦp)πM(p)=πN(Φ(p))(\wedge^2d\Phi_p)\pi_M(p)=\pi_N(\Phi(p))

for every pMp\in M. This condition is contravariant because functions pull back from the target to the source.

Equivalent viewpoints

The bracket and bivector tests are equivalent because the differential of a pullback satisfies d(fΦ)p=dΦp(dfΦ(p))d(f\circ\Phi)_p=d\Phi_p^*(df_{\Phi(p)}). The equality need only be checked locally on coordinate functions and their smooth combinations. The systematic treatment of Poisson morphisms and coinduced structures appears in Vaisman, “Poisson Morphisms, Coinduced Structures, Reduction”.

When both Poisson structures are nondegenerate and arise from symplectic forms, a diffeomorphism is Poisson exactly when it is a , with the compatible sign convention relating the forms and bivectors.

Structure and consequences

Identity maps are Poisson, and the composite of Poisson maps is Poisson. Hence Poisson manifolds and Poisson maps form a category. A Poisson map sends Hamiltonian dynamics contravariantly: the pullback of a Hamiltonian on NN has a that is Φ\Phi-related to the original one whenever the displayed tensor identity applies.

More explicitly, dΦ(XfΦM)=XfNΦd\Phi(X_{f\circ\Phi}^M)=X_f^N\circ\Phi for every fC(N)f\in C^\infty(N). Poisson diffeomorphisms preserve the rank of the Poisson tensor and therefore carry symplectic leaves to symplectic leaves.

Examples and non-examples

The projection M×NMM\times N\to M is Poisson for the product Poisson structure. A constant map with value qNq\in N is Poisson exactly when πN(q)=0\pi_N(q)=0.

A constant map into a positive-dimensional is therefore not Poisson: its differential pushes every bivector to zero, whereas the target Poisson bivector is nonzero. This failure shows that not every smooth map between Poisson manifolds is a Poisson map.

Conventions and scope
References
  1. Izu Vaisman, Lectures on the Geometry of Poisson Manifolds, Progress in Mathematics 118, Birkhäuser, 1994. Publisher record. Relevant: “Poisson Morphisms, Coinduced Structures, Reduction,” pp. 97–114.
  2. Jerrold E. Marsden and Tudor S. Ratiu, Introduction to Mechanics and Symmetry, 2nd ed., Texts in Applied Mathematics 17, Springer, 1999. Publisher record. Relevant: Chapter 10, “Poisson Manifolds.”