The set of all linear maps from where are vector spaces, is called . And is itself a vector space, where the zero function for each acts as the identity vector, and the map is defined as the map that and the map is defined as the one .
Now, given and are vector spaces, we can have linear maps between them. This is the "multilinear nature"
Dual vector space
if is a vector space over , then is called the dual space of . An element of is called a "co-vector".
For example if is the vector space of all polynomials with real entries and real coefficients, the definite integral of an element of from to is an operator call it : , then is a linear map from to , hence , so is a co-vector of .
In general if is a vector space over , is called the dual of . An element of is often called a functional
Hamel Bases
if is a vector space (maybe of infinite dimension), then is a Hamel basis for if for all , there exist a unique finite subset of , and non zero scalars such that .
Co-ordinate projection maps
If is finite dimensional, with basis , Then the 'th projection map is the one that gives the scalar co-efficient of the 'th basis vector when the input vector is written as a linear combination of the basis vectors. that is $$ p_{j}(\lambda_{1}\mathbf{e_{1}}+ \lambda_{2}\mathbf{e_{2}} + \dots \lambda_{n}\mathbf{e_{n}}) = \lambda_{j}$$
If is infinite dimensional, with Hamel basis , then gives the scalar coefficient of the basis vector , when the input vector is written as a unique linear combination of a subset of . that is,
In both cases, the co-ordinate projection maps are linear maps.
In the finite dimensional case $$p_{j}\left( a\sum_{i=1}^n\lambda_{i}\mathbf{e_{i}} +b\sum_{i=1}^n\mu_{i}\mathbf{e_{i}} \right) = a\lambda_{j} + b\mu_{j}$$ and for the infinite dimensional case, I wont write the case-wise breakdown, but okay. Moreover, in both cases the set of all co-ordinate projection maps (also called co-ordinate functionals) are linearly independent vectors in , for the infinite dimension case, consider the functional which is a linear combination of co-ordinate maps being equal to the zero functional. $$ L =\sum_{b \in B}f_{b}p_{b} = \mathbf{0}$$
For any basis , (as L is the zero functional) but Hence , running through all , we notice that each . Hence is linearly independent
Similarly, for the finite dimensional case let $$ T = \sum_{i=1}^n\lambda_{i}p_{i} = \mathbf{0}$$, then , hence running through all ,we have for each . so is a list of linearly independent vectors in . let , for any , Then That is is completely determined by what it does to each of the basis vectors.
Hence we see (beautifully!) that . Notice that .
So the co-ordinate projection functionals are a basis for when is finite dimensional.
Moreover, even if is infinite dimensional, for any , there exists a functional for which . Notice . then simple set then
Also,
Injections into the double dual:
Fix a particular vector . Let .
Define an evaluation map , as . Now,