Definition

Let (M,ωM)(M,\omega_M) and (N,ωN)(N,\omega_N) be . A symplectomorphism from MM to NN is a φ:MN\varphi:M\to N satisfying

φωN=ωM,\varphi^*\omega_N=\omega_M,

where φ\varphi^* denotes . Equivalently, φ\varphi is an invertible . Pointwise, its differential is a :

ωN(dφpu,dφpv)=ωM(u,v)\omega_N(d\varphi_pu,d\varphi_pv)=\omega_M(u,v)

for every pMp\in M and u,vTpMu,v\in T_pM. Thus a symplectomorphism preserves the full symplectic form, not merely the topology, orientation, or associated volume.

Group and local structure

The identity is a symplectomorphism, composites of symplectomorphisms are symplectomorphisms, and the inverse of a symplectomorphism is symplectic. Hence the symplectomorphisms of (M,ω)(M,\omega) form a group, commonly written Symp(M,ω)\operatorname{Symp}(M,\omega). says every two symplectic manifolds of the same dimension are locally symplectomorphic, although global symplectomorphism can be obstructed McDuff–Salamon, Chapter 3.

Dynamics

Whenever a Hamiltonian has a flow defined through time tt, its time-tt map is a symplectomorphism. More generally, a vector field XX generates local symplectomorphisms exactly when LXω=0\mathcal L_X\omega=0. are a distinguished subclass because ιXω\iota_X\omega is exact, not merely closed.

Examples and non-examples

Every A:R2nR2nA:\mathbb R^{2n}\to\mathbb R^{2n} satisfying ATJA=JA^{\mathsf T}JA=J is a symplectomorphism for the standard form. A dilation xcxx\mapsto cx pulls the standard form back to c2ωc^2\omega, so it is symplectic only when c2=1c^2=1. An orientation-preserving, volume-preserving diffeomorphism in dimension greater than two need not preserve the symplectic form.

Conventions and scope

In Hamiltonian mechanics, “canonical transformation” commonly means symplectomorphism, though conventions involving time-dependent or contact transformations may broaden the term. The pullback identity above is the convention used here and in McDuff–Salamon, §1.1.

References
  1. Dusa McDuff and Dietmar Salamon, Introduction to Symplectic Topology, 3rd ed., Oxford University Press, 2017. DOI record. Relevant: §1.1, symplectic manifolds, maps, and diffeomorphisms.
  2. Vladimir I. Arnold, Mathematical Methods of Classical Mechanics, 2nd ed., Springer, 1989. DOI record. Relevant: chapters on symplectic geometry and canonical transformations.