Generalized Eigenspace
Let
be
-square matrix and
be a subspace of
. For any vector
in
, if
, then the subspace
is called an A - invariant.
We write the characteristic polynomial in terms of multiplicity of characteristeic values.
 |
(5.1) |
Here, for the eigenvalues
, we let
Then the following holds.
If you think of the dimension, this can not continue forever. Thus,
and
.
Theorem 5..1
Let
be the
th order square matrix and its characteristic polynomial be (5.1). Then for the generalized eigen space
, the followings hold.
(1) |
 |
(2) |
Generalized eigenvectors for different eigenvalues are linearly independent |
(3) |
 |
Proof
(1) For
, there exists a vector
so that
. Then there is a positive integer
which satisfies
Let
. Then
Since
, there is a positive integer
which satisfies
. But
implies
. This contradicts the condition that for
,
.
(2) Let
be the distinct eigenvalues of
. Then for
, we show by induction that
For
, it is obvious. We assume that
Then by the condition,
We multiply the integer
, which satisfies
, to the equation (**) from the both sides.
Since
is
-invariant,
. Also, from (1), for
,
. Thus,
. Then by the induction hypothesis,
. Therefore,
and we have
.
(3) by the linearly independence shown (2), we have
Also,
. So, to show (3), it is enough to show
い.
The matrix
can be transformed to the following triangular matrix by using unitary matrix
.
Now, we let
Then
is
th vector subspace of
. Also,
implies for every vector
of
, we have
Note that
is regular,
Therefore, let
. Then
is
subspace included in
and obtain the inequality
. Now switching the order of eigenvalues, we have
.
Theorem 5..2
Let
be the
th square matrix and its characteristic polynomial be (*). Then
an be transformed by
to the followings.
Note that
is
th square matrix and its characteristic polynomial is
.
Proof
From
, we take the basis
. Since
is
-invariant, we have
Now let
. Then
is
th square matrix. By the theorem 5.1,
is the basis of
. Therefore, we let
Then
is a regular matrix and
Multiply both sides by
, we obtain the required equation.
Using this relation,
Therefore, if we can show that the eigenvalue of
is
only. Then we can show
and
has the eigenvalues
and the eigenvector corresponds to
are
In other words, if
and let
Then
で
. Therefore,
satisfies
. In other words, it satisfies
. But then this means that
and this contradicts the theorem 5.1.