Cotangent space


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.

Properties edit

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.

Formal definitions edit

Definition as linear functionals edit

Let   be a smooth manifold and let   be a point in  . Let   be the tangent space at  . Then the cotangent space at x is defined as the dual space of  :


Concretely, elements of the cotangent space are linear functionals on  . That is, every element   is a linear map


where   is the underlying field of the vector space being considered, for example, the field of real numbers. The elements of   are called cotangent vectors.

Alternative definition edit

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 fg 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.

This formulation is analogous to the construction of the cotangent space to define the Zariski tangent space in algebraic geometry. The construction also generalizes to locally ringed spaces.

The differential of a function edit

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:

  1.   is a linear map:   for constants   and  ,

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.

The pullback of a smooth map edit

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  .

Exterior powers edit

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.

References edit

  • Abraham, Ralph H.; Marsden, Jerrold E. (1978), Foundations of mechanics, London: Benjamin-Cummings, ISBN 978-0-8053-0102-1
  • Jost, Jürgen (2005), Riemannian Geometry and Geometric Analysis (4th ed.), Berlin, New York: Springer-Verlag, ISBN 978-3-540-25907-7
  • Lee, John M. (2003), Introduction to smooth manifolds, Springer Graduate Texts in Mathematics, vol. 218, Berlin, New York: Springer-Verlag, ISBN 978-0-387-95448-6
  • Misner, Charles W.; Thorne, Kip; Wheeler, John Archibald (1973), Gravitation, W. H. Freeman, ISBN 978-0-7167-0344-0