cotangent bundle


Overview

Let M be a differentiable manifold. Analogously to the construction of the tangent bundleMathworldPlanetmath, we can make the set of covectors on a given manifold into a vector bundleMathworldPlanetmath over M, denoted T*⁢M and called the cotangent bundle of M.

Rigorous Definition

To make this definition precise it is convenient to use the classical definition of a manifold (http://planetmath.org/NotesOnTheClassicalDefinitionOfAManifold). Let M be an n-dimensional differentiable manifold, let {Vα∣α∈𝒜} (each Vα is an open subset of ℝn) be an atlas of M with transition functionsMathworldPlanetmath σα⁢β.

As an atlas for T*⁢(M), we may take {Vα×ℝn∣α∈𝒜}. We may construct transition functions σ′α⁢β as follows:

(σ′α⁢β⁢(x1,…,x2⁢n))i=(σα⁢β⁢(x1,…,xn))i  1≤i≤n
(σ′α⁢β⁢(x1,…,x2⁢n))i+n=∑j=1n∂(σα⁢β(x1,…,xn))i∂⁡xj⁢xj+n  1≤i≤n

For these to be valid transition functions, they must satisfy the three criteria. For a verification that these criteria are satisfied, please see the attachment.

Bundle StructureMathworldPlanetmath

The cotangent bundleMathworldPlanetmath is a G⁢L⁢(n) vector bundle over the manifold M. To substantiate this claim, we must specify a projection map onto the manifold M and local trivializations and transition functions and verify that they satisfies the defining properties of a bundle. In terms of the local coordinates used above, it is easy to describe the projection map π:

π⁢(x1,…,x2⁢n)i=xi

The local trivializations are also somewhat trivial:

ϕα⁢(x1,…,x2⁢n)=xi+n

Finally, the transition functions are given as follows:

gα⁢β⁢(x1,…,x2⁢n)ji=∂(σα⁢β(x1,…xn))i∂⁡xj

For a verification that (T*⁢M,π,ϕα,gα⁢β) satisfies the three criteria for a bundle, please see the attachment.

Properties

The cotangent bundle T*⁢M is the vector bundle dual to the tangent bundle T⁢M. On any differentiable manifold, T*⁢M≅T⁢M (for example, by the existence of a Riemannian metric), but this identification is by no means canonical, and thus it is useful to distinguish between these two objects.

The cotangent bundle to any manifold has a natural symplectic structure given in terms of the Poincaré 1-form, which is in some sense unique. This is not true of the tangent bundle. The existence of a symplectic structure implies that the cotangent bundle is always orientable, even if the original manifold is not.

Title cotangent bundle
Canonical name CotangentBundle
Date of creation 2013-03-22 13:59:02
Last modified on 2013-03-22 13:59:02
Owner rspuzio (6075)
Last modified by rspuzio (6075)
Numerical id 17
Author rspuzio (6075)
Entry type Definition
Classification msc 58A32