Determine how the matrix representation depends on a choice of basis.

Suppose that is an -dimensional vector space equipped with two bases and (as indicated above, any two bases for must have the same number of elements). Taking , Theorem thm:matrep yields the equation where The matrix is referred to as a base transition matrix, and written as . In words, equations (eqn:basechange) and (eqn:basechangematrix) tells us that in order to compute the coordinate vector from , we multiply on the left by the matrix whose column is the coordinate vector of with respect to the basis .

Proof
To show that (a) is true, it is enough to observe that for any coordinate vector there is an equality which implies the equality of matrices . The second statement is clear; is the matrix for which left multiplication by it leaves each coordinate vector unchanged, and the only matrix satisfying this property is the identity matrix. Finally (c) follows from (a) and (b) when .

For vector spaces other than (such as the function space we looked at earlier) where the vectors do not naturally look like column vectors, we always use the above notation when working with their coordinate representations.

However, in the case of , the vectors were defined as column vectors even before discussing coordinate representations. So what should we do here?

The answer is that the vectors in are, by convention, identified with their coordinate representations in the standard basis for . So, for example, in when we wrote what we really meant was that is the vector in with coordinate representation in the standard basis given by .

Because it is very important to keep track of bases whenever determining base transition matrices and computing new coordinate representations, when doing so we will always use base-subscript notation when working with coordinate vectors, even when the vectors are in and are being represented in the standard basis.

The following theorem combines base-transition in both the domain and range, together with matrix representations of linear transformations. It amounts to a “base-transition” for matrix representations of linear transformations.

Let be two bases for , and a linear transformation from to itself. We can consider The representations and of with respect to the bases and . Using the above identities, show that where (hint: apply the above theorem.)

Note: Square matrices which satisfy the equality are called similar. This is an important relation between square matrices, and plays a prominent role in the theory of eigenvalues and eigenvectors as we will see later on.