Digital Signal Processing Reference
In-Depth Information
p
()
() ( )
( )
2
()
γ
mExkxkm
=
= −
a
γ
mn
− +
σδ
m
[6.13]
*
xx
x
xx
n
n
=
1
which we call Yule-Walker equations, which were already mentioned in Chapter 4.
This result shows that the autocorrelation of x ( k ) satisfies the same recursion as the
signal. A large number of estimation methods solve the Yule-Walker equations by
replacing the theoretic autocorrelation ()
by an estimation ()
ˆ xx
γ
m
γ
m
:
xx
1
()
*
()
*
( )
− ⎡
()
()
γ
ˆ
0
γ
ˆ
1
γ
ˆ
p
1
γ
γ
ˆ
1
xx
xx
xx
xx
xx
*
ˆ
2
()
()
( )
ˆ
ˆ
ˆ
γ
1
γ
0
γ
p
ˆ
xx
xx
xx
a
=−
[6.14]
()
γ
ˆ
p
(
)
( )
ˆ
ˆ
γ
p
1
γ
0
xx
xx
xx
ˆ
r
ˆ
-1
x
R
x
ˆ x
It is the autocorrelation method and
is the (estimated) autocorrelation
R
()
matrix. When
ˆ xx γ is the biased estimator of the correlation, the poles are always
inside the unit circle, which is not the case with the non-biased estimator which
gives, however, a better estimation. The Levinson-Durbin algorithm [LEV 47]
provides an order recursive solution of the system [6.14] in O ( p 2 ) computational
burden. In order to reduce the noise influence and to obtain a better estimation, the
system [6.14] can use a larger number of equations (>> p ) and be solved in the least-
squares sense (LS) or in the total least-squares sense (TLS) [VAN 91]. These
methods are called LSYW and TLSYW (see [DUC 98]):
(
)
1
ˆˆ
ˆ
H
H
ˆ
ˆ
LSYW
a
=−
RRRr
xx
xx
(
)
1
ˆˆ
ˆ
H
2
min
H
ˆ
ˆ
TLSYW
a
=−
RR
σ
I
Rr
xx
xx
[6.15]
()
*
( )
()
ˆ
ˆ
ˆ
γ
0
γ
p
1
γ
1
xx
xx
xx
ˆ
ˆ
R
r
=
x
x
(
)
(
)
( )
ˆ
ˆ
ˆ
γ
N
1
γ
N
p
γ
N
xx
0
xx
0
xx
0
ˆ x ⎣ ⎦
Rr , I the identity
matrix and N 0 the number of equations. The value of N 0 should be at most of the
order of
where
σ
is the smaller singular value of the matrix
min
N when the non-biased estimator of the correlation is used so as not to
make correlations with a strong variance intervene.
2
The TLS solution is more efficient than the LS method because it minimizes the
errors in ˆ r and in
ˆ x
R
at the same time, but it presents a disadvantage which we
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