Liouville-preserving diffeomorphisms of cotangent bundles are cotangent lifts #
The cotangent lift T*h : (x, p) ↦ (h x, p ∘ (dh_x)⁻¹) of a smooth diffeomorphism h : M → N
pulls the Liouville form λ_N back to λ_M (Diffeomorph.mpullback_cotangent_liouvilleForm).
This file proves the converse: on Hausdorff manifolds without boundary, every smooth
diffeomorphism ψ : T*M → T*N with ψ^* λ_N = λ_M is the cotangent lift of a unique smooth
diffeomorphism M → N (Diffeomorph.existsUnique_cotangent_eq_of_mpullback_liouvilleForm).
Together with the naturality of λ, this characterizes cotangent lifts among diffeomorphisms
of cotangent bundles (Diffeomorph.exists_cotangent_eq_iff_mpullback_liouvilleForm).
The statement is about the full cotangent bundle, including the zero section. The argument has two steps.
- Fibres go to fibres. A Liouville-preserving
ψcommutes with the positive fibre dilations (Diffeomorph.apply_mk_smul_of_mpullback_liouvilleForm). Letting the dilation factor tend to0and using continuity ofψat the zero section,ψsends the zero covector overxto the zero covector over the base point ofψ (x, p), for every covectorpatx(Diffeomorph.apply_mk_zero_of_mpullback_liouvilleForm). Soψcovers the base mapf x = π (ψ (x, 0)), and it maps the zero section onto the zero section. The same holds forψ⁻¹, sofis a diffeomorphism. - The covector is determined. Since
π_N ∘ ψ = f ∘ π_M, the identityψ^* λ_N = λ_Mevaluated on a tangent vector ofT*Moverv ∈ T_x Mreads(ψ (x, p)) (df_x v) = p v. Everyvlifts, since the projection has surjective derivative (Bundle.mfderiv_proj_surjective). Henceψ (x, p) = (f x, p ∘ (df_x)⁻¹); in particularψis linear on fibres.
Main results #
Diffeomorph.apply_mk_zero_of_mpullback_liouvilleForm: a Liouville-preserving diffeomorphism sends the zero covector over the base point ofzto the zero covector over the base point ofψ z.Diffeomorph.existsUnique_cotangent_eq_of_mpullback_liouvilleForm: a Liouville-preserving diffeomorphism is the cotangent lift of a unique diffeomorphism of the bases.Diffeomorph.exists_cotangent_eq_iff_mpullback_liouvilleForm: a diffeomorphism of cotangent bundles is a cotangent lift exactly when it preserves the Liouville forms.
References #
- A. Cannas da Silva, Lectures on Symplectic Geometry, Lecture Notes in Mathematics 1764, Springer, 2001, Lecture 2 (lifts of diffeomorphisms) and its exercises.
Liouville-preserving diffeomorphisms preserve the zero section and the fibres. Let
ψ : T*M → T*N be a diffeomorphism pulling λ_N back to λ_M. For every covector z, ψ sends
the zero covector over the base point of z to the zero covector over the base point of ψ z.
In particular the base point of ψ z depends only on that of z.
Liouville-preserving diffeomorphisms of cotangent bundles are cotangent lifts. On
Hausdorff manifolds without boundary, a smooth diffeomorphism ψ : T*M → T*N with
ψ^* λ_N = λ_M is the cotangent lift of a unique smooth diffeomorphism h : M → N. Since the
lift covers h, necessarily h x = π (ψ (x, 0)).
Characterization of cotangent lifts. On Hausdorff manifolds without boundary, a smooth
diffeomorphism ψ : T*M → T*N is the cotangent lift of a smooth diffeomorphism M → N exactly
when it pulls the Liouville form λ_N back to λ_M.