Real Invariant Subspaces

Okay, there’s been a bit of a gap while things have gotten hectic around here, but let’s try and get back to work.

When we worked over an algebraically closed field, every polynomial had a root. Applying this to the characteristic polynomial of a linear transformation, we found that it must have a root, which would be definition be an eigenvalue of the transformation. There would then be an eigenvector, which gave a one-dimensional invariant subspace. But when we look at real vector spaces we might not have any one-dimensional invariant subspaces. However, if we don’t we will be sure to have a two-dimensional invariant subspace.

So let’s start with a linear transformation $T:V\rightarrow V$ from a real vector space $V$ of dimension $d$ to itself. Pick any vector $v$ and construct the sequence of images ${Tv}$ , $T^2v$ , and so on up to $T^dv$ . Together with the original vector, these ${d+1}$ vectors cannot be linearly independent, since there are more than $d$ of them. Thus we have a linear relation

$\displaystyle a_0v+a_1Tv+a_2T^2v+...+a_dT^dv=0$

We can regard this as a polynomial in $T$ applied to $v$ , which has real coefficients. We can factor it to write

$\displaystyle c(T-\lambda_1I_V)...(T-\lambda_mI_V)(T^2-\tau_1T+\delta_1I_V)...(T^2-\tau_MT+\delta_MI_V)v$

Note that either $m$ or $M$ could be zero, in which case there are no factors of that form. Also, note that we have no reason to believe that this linear combination has anything to do with the characteristic polynomial, so this factorization is not necessarily giving us eigenvalues or eigenpairs.

All that we can conclude is that at least one of these factors is not injective. If it’s a factor $(T-\lambda_jI_V)$ , then all the factors after that point act on $v$ to give a vector $u$ satisfying

$\displaystyle Tu={\lambda_j}u$

This gives a one-dimensional invariant subspace. On the other hand, if one of the quadratic factors $T^2-\tau_jT+\delta_jI_V$ is not injective, then all the factors after that point act on $v$ to give a vector $u$ satisfying

$\displaystyle T^2u=\tau_jTu-\delta_ju$

which shows that the vectors $u$ and $Tu$ span a two-dimensional invariant subspace, since both basis vectors are sent to a linear combination of each other under the action of $T$ .

Thus we can always find an invariant subspace of dimension one or two. It’s not quite as neat as over the complex numbers, but it’s something we can work with.

About these ads

March 31, 2009 - Posted by John Armstrong | Algebra, Linear Algebra

6 Comments »

Can you prove this result by using the structure theorem for finitely generated modules over principal ideal domains? V is a module over R[X], so V= R[X]/p_1 + … R[X]/p_r (direct sum with the p_i prime powers) and each summand is invariant. But the dimension of the summands might be greater than two if the p_i are proper powers. How does one resolve that?

Comment by Zygmund | March 31, 2009 | Reply
Zygmund, what you’re moving towards is a result I’m also moving towards, but in a more explicit and accessible way. I’d suggest going back and comparing what you’re saying to the decomposition I gave of a complex vector space, and why we needed generalized eigenvectors.

Comment by John Armstrong | March 31, 2009 | Reply
[…] able to find an eigenvector — a one-dimensional invariant subspace — but we know that we can find either a one-dimensional or a two-dimensional invariant subspace . Just like before we get an […]

Pingback by Almost Upper-Triangular Matrices « The Unapologetic Mathematician | April 1, 2009 | Reply
[…] Mathematics In my linear algebra class, we talked about eigenvectors and eigenspaces. This blog post is about a cousin of eigenvectors: invariant subspaces. […]

Pingback by 2 April 2009 « blueollie | April 2, 2009 | Reply
how can u tell that
u, Tu
span a two dimensional subspace? I mean, why cant they be linearly dependent?

Comment by Rafael | March 10, 2010 | Reply
Because, Rafael, if they were linearly dependent then we’d have $Tu=\lambda_ju$ and be in the first case, not the second.

Comment by John Armstrong | March 10, 2010 | Reply

About this weblog

This is mainly an expository blath, with occasional high-level excursions, humorous observations, rants, and musings. The main-line exposition should be accessible to the “Generally Interested Lay Audience”, as long as you trace the links back towards the basics. Check the sidebar for specific topics (under “Categories”).

I’m in the process of tweaking some aspects of the site to make it easier to refer back to older topics, so try to make the best of it for now.

RSS Feeds

RSS - Posts
RSS - Comments
Feedback

Got something to say? Anonymous questions, comments, and suggestions at Formspring.me!
Subjects
Archives

March 2009

M T W T F S S

« Feb Apr »

1

2 3 4 5 6 7 8

9 10 11 12 13 14 15

16 17 18 19 20 21 22

23 24 25 26 27 28 29

30 31
Search for:

The Unapologetic Mathematician

Mathematics for the interested outsider