Digital Signal Processing Reference
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which gives us the variation in eigenvalues ( 15.65 ), while looking outside the diagonal
in ( 15.69 ), one immediately gets matrix B ( 15.66 ) as indeed ( 15.69 ) becomes in this
case for row i , column j :
a t i
0
=
d ii b ij
d jj b ij
A t j .
(15.71)
When d ii =
d jj , this leads to ( 15.67 ), as claimed.
Case 2 some eigenvalues have geometric multiplicity greater than one. Assume now
without loss of generality that g (
d kk ) =
2, with d kk =
d ll ,forsome1
k
=
l
d .
( 15.71 ) shows that t k
t l
A t l =
A t k =
0, which implies that A projects vectors into
the space spanned by eigenvectors
{
t i } i = k , l , so that
{
t k ,
t l }
generates the null space
of A . Picking i
=
k
,
l or j
=
k
,
l in ( 15.71 ) implies
i
,
j
=
k
,
l
:
b kj =
b lj =
b ik =
b il =
0. Hence, in columns k or l , B may only have non-zero values in rows k or l .
But looking at ( 15.70 ) shows that
0, implying d kk =
d ll .
λ kk = λ ll =
d kk =
d ll =
It is immediate to check from ( 15.63 ) that t k and t l are also eigenvectors of
a A .
To finish-up, looking at ( 15.68 ) brings that if the remaining unknowns in columns k
or l in B are non-zero, then t k and t l are collinear, which is impossible.
Θ
Armed with this Lemma, we can prove the following Theorem, in which we
use the decomposition A
= i = 1 a i a i a i
, where a i denotes an eigenvalue with
eigenvector a i .
Theorem 4.
Define e ( Θ )>
0 as the minimum difference between distinct eigenval-
, and d the number of distinct eigenvalues of
ues of
Θ
Θ
. Then, under the first-order
shift setting, the following holds on
ς
( 15.61 ):
ad 2 Tr
4
3
(
A
)
ς
.
(15.72)
e ( Θ )
v i the eigenvector in column i of V in ( 15.63 ). The general
term of V T in row i , column j is:
Proof sketch:
We denote
v i
t j , but it comes from the definition of B
t i + k b ki t k , which yields
v i
b ji
v i =
t j =
=
in ( 15.68 ) that
if i
j (and 1
otherwise); so:
F
V T
V T
ς =
I
(
) · (
)
=
B
·
B
F
a t i A t j
d ii
4
=
,
d jj
π( i , j )
where
π(
i
,
j
)
is the Boolean predicate
( g (
d ii ) =
1
) ( g (
d jj ) =
1
) (
i
=
j
)
.
We finally get:
 
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