Some Representations of the General Linear Group
Sorry for the delays, but it’s the last week of class and everyone came back from the break in a panic.
Okay, let’s look at some examples of group representations. Specifically, let’s take a vector space and consider its general linear group
.
This group comes equipped with a representation already, on the vector space itself! Just use the identity homomorphism
We often call this the “standard” or “defining” representation. In fact, it’s easy to forget that it’s a representation at all. But it is.
As with any other group, we have dual representations. That is, we immediately get an action of on
. And we’ve seen it already! When we talked about the coevaluation on vector spaces we worked out how a change of basis affects linear functionals. What we found is that if
is our action on
, then the action on
is by the transpose — the dual — of
. And this is exactly the dual representation.
Also, as with any other group, we have tensor representations — actions on the tensor power for any number
of factors of
. How does this work? Well, every vector in
is a linear combination of vectors of the form
, where each
. And we know how to act on these: just act on each tensorand separately. That is,
Then we just extend this action by linearity to all of .

Out of curiosity: where are you heading with this? Were you planning to discuss Schur-Weyl duality?
Actually, I’m going to mention it tomorrow. But I’m not going to actually prove it, or use it as such. What I am going to do is introduce a particular representation that many readers may already be familiar with, but without picking a basis!
[...] Symmetric Group Representations Tuesday, we talked about tensor powers of the standard representation of . Today we’ll look at some representations of the symmetric [...]
Pingback by Some Symmetric Group Representations « The Unapologetic Mathematician | December 4, 2008 |
[...] tomorrow I want to take last Friday’s symmetrizer and antisymmetrizer and apply them to the tensor representations of , which we know also carry symmetric group representations. Specifically, the th tensor power [...]
Pingback by Symmetric Tensors « The Unapologetic Mathematician | December 22, 2008 |
[...] project by considering antisymmetric tensors today. Remember that we’re starting with a tensor representation of on the tensor power , which also carries an action of the symmetric group by permuting the [...]
Pingback by Antisymmetric Tensors « The Unapologetic Mathematician | December 23, 2008 |
[...] vector space. But remember that this isn’t just a vector space. The tensor power is both a representation of and a representation of , which actions commute with each other. Our antisymmetric tensors are [...]
Pingback by The Determinant « The Unapologetic Mathematician | December 31, 2008 |
[...] each degree. And if is invertible, so must be its image under each functor. These give exactly the tensor, symmetric, and antisymmetric representations of the group , if we consider how these functors act [...]
Pingback by Functoriality of Tensor Algebras « The Unapologetic Mathematician | October 28, 2009 |