Eigenvalue-Eigenvector Examples
Math 5718 - Spring 2001
These notes consist of examples of the various cases that arise in
working with eigenvalues and eigenvectors. The examples are
intended to illustrate the theorems of Chapter 5. Recall that the
author of the text approaches the eigenvalue problem through
invariant subspaces, without using the traditional definition of
an eigenvalue (involving determinants and characteristic
polynomials). You may certainly compute eigenvalues in the usual
way, if it helps you to construct examples and improve your
understanding. We also know that the eigenvalues of an upper
triangular matrix (which includes diagonal matrices) are the
diagonal elements of the matrix.
Example 1: Consider the matrix
,
where
,
given by
The eigenvalues,
,
and
,
are on the
diagonal of this upper triangular matrix. To find the
eigenvectors, we find a basis for the invariant subspaces
.
You should verify that
and
The eigenvalues are distinct and the corresponding eigenvectors are linearly independent. Each eigenvalue has an invariant subspace of dimension 1.
Referring to the proof of Theorem 5.10, you can also verify that
p(T)=T3-6T2+11T-6I = (T-I)(T-2I)(T-3I)=0.
This roots of this polynomial (soon to be called the
characteristic polynomial) are the eigenvalues.
Example 2: Consider the matrix
,
where
,
given by
The eigenvalues,
and
,
are on the diagonal. To
find the eigenvectors, we find a basis for the invariant subspaces
.
You should verify that
and
In this case, but not always, the double eigenvalue has an invariant subspace of dimension 2. This example illustrates the provisions of Proposition 5.21 of the text: V has a basis consisting of eigenvectors,
,
where Ui is the span of the ith eigenvector,
and
Referring to the proof of Theorem 5.10, you can also verify that
p(T)=T3-3T2-T+3I = (T-I)2(T-3I)=0.
This roots of this polynomial are the eigenvalues.
Example 3: Consider the matrix
,
where
,
given by
The eigenvalues,
and
,
are on the diagonal of
this upper triangular matrix. To find the eigenvectors, we find a
basis for the invariant subspaces
.
You
should verify that
and
In this case, the double eigenvalue has an invariant subspace of dimension 1.
Referring to the proof of Theorem 5.10, you can also verify that
p(T)=T3-3T2-T+3I = (T-I)2(T-3I)=0.
This polynomial is identical to the polynomial of Example 2, because the eigenvalues of the two matrices are the same.
Example 4: Consider the matrix
,
where
,
given by
Because the matrix is not upper triangular, the eigenvalues are
not so evident. There are three invariant subspaces corresponding
to
,
and
.
To find the eigenvectors,
we find a basis for the invariant subspaces
.
You should verify that
and
The three distinct eigenvalues correspond to three linearly independent eigenvectors. Each eigenvalue has an invariant subspace of dimension 1.
Referring to the proof of Theorem 5.10, you can also verify that
p(T)=T3-4T2-15T+18I = (T+3I)(T-I)(T-6I)=0.
Again, the roots of this polynomial are the eigenvalues.
Example 5: Consider the matrix given by
This matrix has only one eigenvalue,
,
and it has an
invariant subspace,
,
of dimension 1.
The main point here is that zero can be an eigenvalue and a matrix
can be deficient in eigenvalues and eigenvectors.
Example 6: Consider the matrix
,
where
or
,
given by
Over the complex numbers, there are two distinct eigenvalues,
.
Associated with each eigenvalue is an
invariant subspace of T of dimension 1,
.
The eigenvectors are multiples of
.
Over the real numbers, there are no (real) eigenvalues. There is
an invariant subspace of T, namely
.
In
fact, you can verify that T2+4I=0, meaning that the invariant
subspace is
.
Example 7: Consider the matrix
,
where
or
,
given by
If you compute the eigenvalues explicitly, they turn out to be
and
.
If we were working over the
complex numbers, there would be three invariant subspaces,
,
and there would be three linearly independent
eigenvectors (with complex elements) associated with the
eigenvalues. However, over the real numbers, there are two
invariant subspaces. You can verify that
and
In this case, there is an invariant subspace of dimension 2, with
a basis
v1=(1,0,0)T and
v2=(0,1,0)T. Notice that v1 and
v2 are not themselves eigenvectors; however, Tv1=v2 and
Tv2=v1. Consistent with Theorem 5.26, we are assured of one
real eigenvalue. Referring to the proof of Theorem 5.24, you can
also verify that
p(T)=T3-2T2+T-2I = (T2+I)(T-2I) =0.