Digital Signal Processing Reference
In-Depth Information
2
( )
(
)
(
)
Σ
m
,
=
2
σ
⎡
c
+
m
+
c
−
m
⎤
⎣
⎦
ss
ss
[3.20]
(
{ }
⎡
⎤
4
(
)
4
4
() ( )
+
σδ
−
mb
+
n
−
2
σ δ δ
m
E
⎢
⎥
⎣
⎦
Finally, we would like to mention that very general theoretical results, as they
concern signals that are a combination of deterministic and random components
(stationary or non-stationary), were published by Dandawaté and Giannakis [DAN
95]. This last article makes it possible to include a very large class of signals and
provides analytical expressions of asymptotic distributions of moment estimates.
Finally, the reader is asked to read [DAN 95, LAC 97] for the analysis of estimator
of higher order moments.
3.3. Periodogram analysis
The periodogram is a natural estimation tool for the power spectral density. Let
us recall that its expression is:
2
N
−
1
N
−
1
1
∑
∑
()
()
−
j
2
π
f
()
−
j
2
π
mf
If
=
xne
=
γ
ˆ
me
[3.21]
xx
N
(
)
n
=
0
m
=− −
N
1
where:
Nm
−−
1
1
∑
()
()( )
ˆ
γ
m
=
x n x n
+
m
xx
N
n
=
0
designates the biased estimator of the correlation function. The objective of this
section is to derive the asymptotic properties of
I
(
f
) for a real signal. Firstly we
calculate the bias of this estimator. The periodogram mean can directly be written
as:
N
−
1
⎛
m
⎞
∑
{
}
()
()
−
j
2
π
mf
If
=
1
−
γ
me
E
⎜
⎟
xx
N
⎝
⎠
(
)
mN
=− −
1
1/ 2
∫
() ( )
=
SvWfv v
−
x
−
1/ 2
2
1
(
)
⎡
sin
sin
π
π
fN
f
⎤
where
()
Wf
=
⎦
is the Fourier transform of the triangular window.
⎢
⎥
( )
N
⎣
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