Inlinear algebra, the transpose of alinear map between two vector spaces, defined over the samefield, is an induced map between thedual spaces of the two vector spaces. Thetranspose oralgebraic adjoint of a linear map is often used to study the original linear map. This concept is generalised byadjoint functors.
Let denote thealgebraic dual space of a vector space. Let and be vector spaces over the same field. If is alinear map, then itsalgebraic adjoint ordual,[1] is the map defined by. The resulting functional is called thepullback of by.
Thecontinuous dual space of atopological vector space (TVS) is denoted by. If and are TVSs then a linear map isweakly continuous if and only if, in which case we let denote the restriction of to. The map is called thetranspose[2] oralgebraic adjoint of. The following identity characterizes the transpose of:[3]where is thenatural pairing defined by.
The assignment produces aninjective linear map between the space of linear operators from to and the space of linear operators from to. If then the space of linear maps is analgebra undercomposition of maps, and the assignment is then anantihomomorphism of algebras, meaning that. In the language ofcategory theory, taking the dual of vector spaces and the transpose of linear maps is therefore acontravariant functor from the category of vector spaces over to itself. One can identify with using the natural injection into the double dual.
Suppose now that is a weakly continuous linear operator betweentopological vector spaces and with continuous dual spaces and, respectively. Let denote the canonicaldual system, defined by where and are said to beorthogonal if. For any subsets and, let denote the (absolute)polar of in (resp.of in).
If and are convex, weakly closed sets containing the origin then implies.[7]
Suppose and aretopological vector spaces and is a weakly continuous linear operator (so). Given subsets and, define theirannihilators (with respect to the canonical dual system) by[6]
and
Thekernel of is the subspace of orthogonal to the image of:[7]
The linear map isinjective if and only if its image is a weakly dense subset of (that is, the image of is dense in when is given the weak topology induced by).[7]
The transpose is continuous when both and are endowed with theweak-* topology (resp. both endowed with thestrong dual topology, both endowed with the topology of uniform convergence on compact convex subsets, both endowed with the topology of uniform convergence on compact subsets).[8]
Let be a closed vector subspace of a Hausdorff locally convex space and denote the canonical quotient map byAssume is endowed with thequotient topology induced by the quotient map. Then the transpose of the quotient map is valued in andis a TVS-isomorphism onto. If is aBanach space then is also anisometry.[6] Using this transpose, every continuous linear functional on the quotient space is canonically identified with a continuous linear functional in the annihilator of.
Let be a closed vector subspace of a Hausdorff locally convex space. If and if is a continuous linear extension of to then the assignment induces a vector space isomorphismwhich is an isometry if is a Banach space.[6]
Denote theinclusion map byThe transpose of the inclusion map iswhose kernel is the annihilator and which is surjective by theHahn–Banach theorem. This map induces an isomorphism of vector spaces
If the linear map is represented by thematrix with respect to two bases of and, then is represented by thetranspose matrix with respect to the dual bases of and, hence the name. Alternatively, as is represented by acting to the right on column vectors, is represented by the same matrix acting to the left on row vectors. These points of view are related by the canonical inner product on, which identifies the space of column vectors with the dual space of row vectors.
The identity that characterizes the transpose, that is,, is formally similar to the definition of theHermitian adjoint, however, the transpose and the Hermitian adjoint are not the same map. The transpose is a map and is defined for linear maps between any vector spaces and, without requiring any additional structure. The Hermitian adjoint maps and is only defined for linear maps between Hilbert spaces, as it is defined in terms of theinner product on the Hilbert space. The Hermitian adjoint therefore requires more mathematical structure than the transpose.
However, the transpose is often used in contexts where the vector spaces are both equipped with anondegenerate bilinear form such as the Euclideandot product or anotherrealinner product. In this case, the nondegenerate bilinear form is oftenused implicitly to map between the vector spaces and their duals, to express the transposed map as a map. For a complex Hilbert space, the inner product is sesquilinear and not bilinear, and these conversions change the transpose into the adjoint map.
More precisely: if and are Hilbert spaces and is a linear map then the transpose of and the Hermitian adjoint of, which we will denote respectively by and, are related. Denote by and the canonical antilinear isometries of the Hilbert spaces and onto their duals. Then is the following composition of maps:[10]