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finite-dimensional spectral theory is that the eigenvalues of a matrix A are,
respecting multiplicities, precisely the roots of the characteristic polynomial
χ B
ðÞ:¼ det A λ
ð
I
Þ:
It turns out that the characteristic polynomial of a rank-1 modification of a
diagonal matrix has a closed-form representation.
n .
Proposition 8.3 Let
Λ
: ¼ diag(
λ 1 ,
...
,
λ n ) be a real diagonal matrix and x
∈ R
+ xx T is given by
Then the characteristic polynomial of
Λ
¼ det
Þ 1 x
Λ þ xx T
1 þ x T
det
λ
I
ð
Λ λ
I
Þ
ð
Λ λ
I
!
!
Y
1 þ X
n
1 λ i λ
n
x i
λ i λ
¼
ð
Þ
:
1
A proof may be found in, e.g., [GE94].
For the sake of simplicity, our discussion is restricted to the case where:
1.
λ n are distinct.
2. The spectra of
λ 1 ,
...
,
+ xx T are disjoint.
Λ
and
Λ
For a more general treatment, please consult [BNS78].
If the second of the above conditions holds, then λ
+ xx T if
is an eigenvalue of
Λ
and only if
1
Λ λ
1 þ x T
I
x ¼ 0
:
ð 8
:
16 Þ
Hence, the eigenvalues of the rank-1 modification may be obtained by solving
the secular equation ( 8.16 ). To do so, we may exploit the following insight.
Proposition 8.4 (cf. [GE94]) The eigenvalues λ 1 ... λ n of
+ xx T satisfy the
Λ
interlacing property
λ i λ i λ i 1 ,
i ¼ 2,
...
, n
:
By virtue of this observation, we are given intervals in which precisely one
eigenvalue is located. How should we proceed to solve ( 8.16 )? The most straight-
forward way consists in deploying a bisection method. Since Proposition 8.4 pro-
vides suitable initializations, such a method is guaranteed to converge. The rate,
however, is only q -linear. A method exhibiting q -quadratic convergence is
Newton-Raphson. Unfortunately, we are not in a position to guarantee convergence
thereof because it may “leap” over the singularities and thus out of the search
intervals in an early stage. A more sophisticated method, again, has been proposed
in [BNS78]: the rational function on the right-hand side of ( 8.16 ) is iteratively
approximated by low-degree rational functions the roots of which are available in
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