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on the other hand, depends on the Hermitian correlation only:
{ V xx [ k 1 1 )
, V xx [ k 2 2 )
}
cov
µ 2 φ
φ [ m 2 2 ]e j( µ 1 θ 1 µ 2 θ 2 )
=
[ m 1 1 ]
m 1
m 2
µ 1
×{
r xx [ k 1 +
m 1 + µ 1 ,
k 2
k 1 +
m 2
m 1 + µ 2 µ 1 ]
×
r xx [ k 1 +
m 1 ,
k 2
k 1 +
m 2
+
r xx [ k 1 +
m 1 ,
k 2
k 1 +
m 2
m 1 + µ 2 ]
m 1 ]
×
r xx [ k 1 +
m 1 + µ 1 ,
k 2
k 1 +
m 2
m 1 µ 1 ]
} .
We can derive the following approximate expression for the variance of the HR-
TFD estimator, assuming analytic and quasi-stationary signals whose time duration of
stationarity is much greater than the duration of correlation:
π
0 |
{ V xx [ k
2
2
}≈
ω
|
|
|
var
)
[ m
k
)
V xx [ k
)
m
d
ω
| V xx [ k
[ m
2
+
[ m
k
ω
)
k
+ ω
)
)
|
π .
(9.105)
2
However, the same simplifying approximation of large duration of stationarity leads to a
vanishing CR-TFD estimator because stationary analytic signals have zero complemen-
tary correlation. This result should not be taken as an indication that the CR-TFD is not
important for analytic signals. Rather it shows that the assumption of quasi-stationarity
with large duration of stationarity is a rather crude approximation to the general class of
nonstationary signals.
9.4
Rotary-component and polarization analysis
In Section 9.3.1 , we determined the LMMSE estimator of the time-domain signal at a
fixed time instant t from the frequency-domain representation at a fixed frequency f .
This showed us how well the signal can be approximated from clockwise or counter-
clockwise turning circles (phasors). It thus seems natural to ask how well the signal can
be approximated from ellipses , which combine the contributions from clockwise and
counterclockwise circles. This framework will allow us to extend rotary-component and
polarization analysis from the stationary case, described in Section 8.4 , to a nonstation-
ary setting. 12 We thus construct a WLMMSE estimator of x ( t ), for fixed t , from the
frequency-domain representation at
+
f and
f , where throughout this entire section
f shall denote a fixed nonnegative frequency:
( f )e j2 π ft
ξ ( f )e j2 π ft
x f ( t )
=
W 1 ( t
,
f )d
ξ
+
W 2 ( t
,
f )d
f )e j2 π ft
ξ (
f )e j2 π ft
+
W 1 ( t
,
f )d
ξ
(
+
W 2 ( t
,
f )d
.
(9.106)
 
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