In differential geometry, the cotangent space is a vector space associated with a point on a smooth (or differentiable) manifold ; one can define a cotangent space for every point on a smooth manifold. Typically, the cotangent space, is defined as the dual space of the tangent space at , , although there are more direct definitions (see below). The elements of the cotangent space are called cotangent vectors or tangent covectors.
All cotangent spaces at points on a connected manifold have the same dimension, equal to the dimension of the manifold. All the cotangent spaces of a manifold can be "glued together" (i.e. unioned and endowed with a topology) to form a new differentiable manifold of twice the dimension, the cotangent bundle of the manifold.
The tangent space and the cotangent space at a point are both real vector spaces of the same dimension and therefore isomorphic to each other via many possible isomorphisms. The introduction of a Riemannian metric or a symplectic form gives rise to a natural isomorphism between the tangent space and the cotangent space at a point, associating to any tangent covector a canonical tangent vector.
In some cases, one might like to have a direct definition of the cotangent space without reference to the tangent space. Such a definition can be formulated in terms of equivalence classes of smooth functions on . Informally, we will say that two smooth functions f and g are equivalent at a point if they have the same first-order behavior near , analogous to their linear Taylor polynomials; two functions f and g have the same first order behavior near if and only if the derivative of the function f − g vanishes at . The cotangent space will then consist of all the possible first-order behaviors of a function near .
Let be a smooth manifold and let x be a point in . Let be the ideal of all functions in vanishing at , and let be the set of functions of the form , where . Then and are both real vector spaces and the cotangent space can be defined as the quotient space by showing that the two spaces are isomorphic to each other.
Let be a smooth manifold and let be a smooth function. The differential of at a point is the map
where is a tangent vector at , thought of as a derivation. That is is the Lie derivative of in the direction , and one has . Equivalently, we can think of tangent vectors as tangents to curves, and write
In either case, is a linear map on and hence it is a tangent covector at .
We can then define the differential map at a point as the map which sends to . Properties of the differential map include:
The differential map provides the link between the two alternate definitions of the cotangent space given above. Since for all there exist such that , we have, i.e. All function in have differential zero, it follows that for every two functions , , we have . We can now construct an isomorphism between and by sending linear maps to the corresponding cosets . Since there is a unique linear map for a given kernel and slope, this is an isomorphism, establishing the equivalence of the two definitions.
Just as every differentiable map between manifolds induces a linear map (called the pushforward or derivative) between the tangent spaces
every such map induces a linear map (called the pullback) between the cotangent spaces, only this time in the reverse direction:
The pullback is naturally defined as the dual (or transpose) of the pushforward. Unraveling the definition, this means the following:
where and . Note carefully where everything lives.
If we define tangent covectors in terms of equivalence classes of smooth maps vanishing at a point then the definition of the pullback is even more straightforward. Let be a smooth function on vanishing at . Then the pullback of the covector determined by (denoted ) is given by
That is, it is the equivalence class of functions on vanishing at determined by .
The -th exterior power of the cotangent space, denoted , is another important object in differential and algebraic geometry. Vectors in the -th exterior power, or more precisely sections of the -th exterior power of the cotangent bundle, are called differential -forms. They can be thought of as alternating, multilinear maps on tangent vectors. For this reason, tangent covectors are frequently called one-forms.