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Theorem 8.4.1 (Gershgorin)
For
![$A=[a_{ij}]\in \hbox{{\sf I}\kern-.4em\hbox{\sf C}}^{n\times n} $](img37.gif)
,
let
Then
- (a)
- each eigenvalue lies in the union of discs
,
- (b)
- each eigenvalue lies in the union of discs
,
- (c)
- if the union of m of either of these sets of discs is disjoint
from the remainder of that set, then this union of m discs contains
just m eigenvalues of A (counting multiplicities).
Proof. - (a)
- For any eigenvalue
of A and corresponding eigenvector
,
we have
.
Writing this in component form
and rearranging we find
Now choose the particular value of i for which
,
then
The result follows, since the choice of eigenvalue was arbitrary.
- (b)
- This follows by applying (a) to AT.
- (c)
- Consider the family of matrices A(t)=D+tB, where D is the
diagonal part of A and B is the rest. Each eigenvalue lies in the
union of discs
.
As t runs
from 0 to 1, A(t) goes from D to A. The coefficients of the
characteristic equation are polynomials in t and the roots (i.e.
the eigenvalues of A) are continuous functions of the coefficients and
hence of t.
When t=0, the discs are just points, each corresponding to an
eigenvalue; as t increases, two of the discs intersect, and the
eigenvalues must stay within the union, since otherwise they would have
to move discontinuously in order to go into another non-intersecting
disc. Thus, each intersection brings with it just one eigenvalue.
This concludes the proof.
Corollary 8.4.2
With the hypotheses of the theorem
Proof.
, so
, etc.Example.
.
The eigenvalues lie in the union of
.
The characteristic equation is actually
giving the eigenvalues as i,3,6. The corollary gives
.
We consider the effect of a small perturbation of A into
upon the
eigenvalues of A, where A and B are made comparable in size by
scaling them so that the moduli of their maximum elements are bounded
by 1. We assume that A is nondefective, with right and left
eigenvectors
and
, both sets of which are linearly independent, and
which are scaled so that
for
.
Let
, so that, with the help of the Schwarz inequality,
Let
.
Then, using the Schwarz inequality again,
where the last result is from exercise 36.
Let
, then
, since
, using the biorthogonality property. Now
Gershgorin gives the discs containing the eigenvalues of
and hence of
as
The condition of the ith eigenvalue clearly depends on |si|; if
this is small, it suggests that the calculation of
is
ill-conditioned.
Lemma 8.4.3
Let
![$\Lambda =\, {\rm diag}\, [\lambda _i]\in \hbox{{\sf I}\kern-.4em\hbox{\sf C}}^{n\times n}$](img68.gif)
.
Then

.
Proof.
.
Theorem 8.4.4
Let

and
A be nondefective,
with eigenvalues

.
If

is an eigenvalue of

,
where

is a
positive scalar, then for some
i
where

is the spectral condition number of
A.
Proof. Let X be the matrix whose columns are the eigenvectors
of A. Then if
This implies that
has an eigenvalue -1, so
which implies that
Since the case when
also satisfies this
inequality, it is true in that case also.If A is Hermitian, we can scale X to be unitary and so
, which shows that an Hermitian matrix is as well-conditioned as
possible for the eigenvalue problem also.
Next: a posteriori Error bounds
Up: The Eigenproblem
Previous: Right and Left Eigenvectors
John Gilbert
1999-03-01