General Linear Groups — Generally
Monday, we saw that the general linear groups are matrix groups, specifically consisting of those whose columns are linearly independent. But what about more general vector spaces?
Well, we know that every finite-dimensional vector space has a basis, and is thus isomorphic to , where
is the cardinality of the basis. So given a vector space
with a basis
of cardinality
, we have the isomorphism
defined by
and
.
This isomorphism of vector spaces then induces an isomorphism of their automorphism groups. That is, . Given an invertible linear transformation
, we can conjugate it by
to get
. This has inverse
, and so is an element of
. Thus (not unexpectedly) every invertible linear transformation from a vector space
to itself gets an invertible matrix.
But this assignment depends essentially on the arbitrary choice of the basis for
. What if we choose a different basis
? Then we get a new transformation
and a new isomorphism of groups
. But this gives us an inner automorphism of
. Given a transformation
, we get the transformation
This composite sends
to itself, and it has an inverse. Thus changing the basis on
induces an inner automorphism of the matrix group
.
Now let’s consider a linear transformation . We have two bases for
, and thus two different matrices — two different elements of
— corresponding to
:
and
. We get from one to the other by conjugation with
:
And what is this transformation ? How does it act on a basis vector in
? We calculate:
where expresses the vectors in one basis for
in terms of those of the other. That is, the
th column of the matrix
consists of the components of
written in terms of the
. Similarly, the inverse matrix
with entries
, writes the
in terms of the
:
.
It is these “change-of-basis” matrices that effect all of our, well, changes of basis. For example, say we have a vector with components
. Then we can expand this:
So our components in the new basis are .
As another example, say that we have a linear transformation with matrix components
with respect to the basis
. That is,
. Then we can calculate:
and we have the new matrix components .
