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on the other hand, depends on the Hermitian correlation only:
{
V
xx
[
k
1
,θ
1
)
,
V
xx
[
k
2
,θ
2
)
}
cov
µ
2
φ
φ
∗
[
m
2
,µ
2
]e
−
j(
µ
1
θ
1
−
µ
2
θ
2
)
=
[
m
1
,µ
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
,θ
}≈
−
,θ
−
ω
|
|
,ω
|
var
)
[
m
k
)
V
xx
[
k
)
m
d
ω
|
V
xx
[
k
∗
[
m
2
+
[
m
−
k
,θ
−
ω
)
−
k
,θ
+
ω
)
,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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