Consider the real vector space of all height 3 column vectors, and the real vector space of all height 3 row vectors. These are different vector spaces but they are essentially the same: there’s no vector space property which one has but the other doesn’t.
A way to make this precise is to observe that there is a bijective linear map between them, namely the transpose which sends to .
Linear maps which are bijections are called vector space isomorphisms, or just isomorphisms.
If there is an isomorphism , we say that and are isomorphic and write .
Isomorphic vector spaces share the same vector space properties — for example, they always have the same dimension.
If then .
There’s a linear bijection . , so applying the rank-nullity theorem . Since we get , but is onto so and . ∎
If is a finite-dimensional -vector space with a basis then every can be written uniquely as for some . The column vector
is called the coordinate vector of with respect to . We can use this idea to define an isomorphism between and .
Let be a -vector space with basis . Define to be the function that sends to its coordinate vector . Then is a vector space isomorphism.
is called the coordinate isomorphism with respect to .
First we have to show it is linear.
Let and let and , so that and . Then , so
Let and . If so that , then so .
Now we have to show it is injective and surjective.
If then by definition . Therefore and by Proposition 4.14.3, is injective.
Any vector in is the image of under .
∎
In particular, every finite-dimensional vector space is isomorphic to a space of column vectors.
Suppose we have -vector spaces of dimensions and with bases and a linear map . We have coordinate isomorphisms and and a matrix . What is the relationship between and the linear map given by left-multiplication by ?
In the notation above, for any we have .
Let , so that . Notice that this says is , the th column of . The coordinate vector is the th standard basis vector , so which equals the th column of . Therefore
(4.8) |
Let and write so that . Then
(4.8) | ||||
∎
We can now answer the following natural question: if and are two bases of the finite-dimensional vector space and , what is the relationship between and ? Using the previous theorem applied to the identity map ,