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TauCeti.Geometry.Symplectic.Cotangent.Bundle.Domain

The unit codisc bundle is a Liouville domain #

Let M be a compact smooth Riemannian manifold without boundary, with cotangent bundle T*M = TauCeti.CotangentBundle I M, Liouville form λ = p dq and canonical symplectic form ω = -dλ, which is nondegenerate (TauCeti.CotangentBundle.isSymplectic_symplecticForm). The radial field Z = p ∂_p, the Euler vector field of the bundle, is the Liouville field of the primitive -λ of ω (TauCeti.CotangentBundle.symplecticForm_interior_vectorBundleEulerField).

The unit codisc bundle D*M = {‖p‖ ≤ 1} is compact, and it is the sublevel set of the norm of covectors, which is continuous on T*M and smooth off the zero section. Along the fibre ray t ↦ t • z the norm is t ↦ |t| ‖z.2‖, so the differential of the norm sends Z to ‖z.2‖ (TauCeti.CotangentBundle.mfderiv_norm_snd_vectorBundleEulerField), which is 1 > 0 on the unit cosphere bundle S*M = {‖p‖ = 1}. Hence (D*M, -λ) is a Liouville domain in (T*M, ω) with Liouville field p ∂_p (TauCeti.CotangentBundle.isLiouvilleDomain_codiscBundle). It is the Liouville domain on which the symplectic homology and the capacities of cotangent bundles are computed; its boundary is S*M, of restricted contact type (TauCeti.CotangentBundle.isRestrictedContactType_cosphereBundle).

The flow of p ∂_p is the fibre dilation p ↦ e^t p, defined for all time, and it shrinks every covector into D*M. So T*M is the completion of D*M (TauCeti.CotangentBundle.isLiouvilleCompletion_codiscBundle): every covector outside D*M is e^t p for exactly one unit covector p and one time t > 0.

Main results #

References #

The unit codisc bundle is a Liouville domain. For a compact smooth Riemannian manifold M without boundary, the unit codisc bundle D*M is a Liouville domain in T*M for the canonical symplectic form ω = -dλ, with primitive -λ: its Liouville field, the radial field p ∂_p, points strictly outwards along the unit cosphere bundle, the level ‖p‖ = 1 of the norm of covectors.

The cotangent bundle is the completion of the unit codisc bundle. For a compact smooth Riemannian manifold M without boundary, T*M is a completion of the Liouville domain D*M: the flow p ↦ e^t p of its Liouville field p ∂_p is defined for all time, and carries every covector into D*M.