In mathematics, the tensor-hom adjunction is that the tensor product
and hom-functor
form an adjoint pair:

This is made more precise below. The order of terms in the phrase "tensor-hom adjunction" reflects their relationship: tensor is the left adjoint, while hom is the right adjoint.
General statement[edit]
Say R and S are (possibly noncommutative) rings, and consider the right module categories (an analogous statement holds for left modules):

Fix an
-bimodule
and define functors
and
as follows:


Then
is left adjoint to
. This means there is a natural isomorphism

This is actually an isomorphism of abelian groups. More precisely, if
is an
-bimodule and
is a
-bimodule, then this is an isomorphism of
-bimodules. This is one of the motivating examples of the structure in a closed bicategory.[1]
Counit and unit[edit]
Like all adjunctions, the tensor-hom adjunction can be described by its counit and unit natural transformations. Using the notation from the previous section, the counit

has components

given by evaluation: For


The components of the unit


are defined as follows: For
in
,

is a right
-module homomorphism given by

The counit and unit equations can now be explicitly verified. For
in
,

is given on simple tensors of
by

Likewise,

For
in
,

is a right
-module homomorphism defined by

and therefore

The Ext and Tor functors[edit]
The Hom functor
commutes with arbitrary limits, while the tensor product
functor commutes with arbitrary colimits that exist in their domain category. However, in general,
fails to commute with colimits, and
fails to commute with limits; this failure occurs even among finite limits or colimits. This failure to preserve short exact sequences motivates the definition of the Ext functor and the Tor functor.
See also[edit]
References[edit]
- ^
May, J.P.; Sigurdsson, J. (2006). Parametrized Homotopy Theory. A.M.S. p. 253. ISBN 0-8218-3922-5.