Digital Signal Processing Reference
In-Depth Information
The beamformer weight vector
w
is chosen with an aim that it is statistically opti-
mum in some sense. Naturally, different design objectives lead to different beamfor-
mer weight vectors. For example, the weight vector for the classic beamformer is
a
a
H
a
w
BF
W
where
a ¼ a
(
~
u
) denotes the array response for fixed look direction
u
. The classic
Capon's [7] MVDR beamformer chooses
w
as the minimizer of the output power
while constraining the beam response along a specific look direction
u
of the SOI
to be unity
mi
w
w
H
C
(
z
)
w
subject to
w
H
a ¼
1
:
The well-known solution to this constrained optimization problem is
w
C
(
z
)
W
C
(
z
)
1
a
a
H
C
(
z
)
1
a
:
(2
:
29)
Observe that Capon's beamformer weight vector is data dependent whereas the classic
beamformer weight
w
BF
is not, that is,
w
C
(
) is a statistical functional as its value
depends on the distribution
F
of
z
via the covariance matrix
C
(
F
). The spectrum
(2.28) for the classic and Capon's beamformers can now be written as
P
BF
(
u
)
W
a
(
u
)
H
C
(
z
)
a
(
u
)
(2
:
30)
P
CAP
(
u
)
W
[
a
(
u
)
H
C
(
z
)
1
a
(
u
)]
1
(2
:
31)
respectively. (See Section 6 in [55]). Note that MVDR beamformers do not make any
assumption on the structure of the covariance matrix (unlike the subspace-methods of
the next section) and hence can be considered as a “nonparametric method” [55].
In practice, the DOA estimates for the classic and Capon's beamformer are calcu-
lated as the
d
highest peaks in the estimated spectrums
P
BF
(
u
) and
P
CAP
(
u
), where the
true unknown covariance matrix
C
(
z
) is replaced by its conventional estimate, the
SCM
C
. An intuitive approach in obtaining robust beamformer DOA estimates is to
use robust estimators instead of the SCM in (2.30) and (2.31), for example, the
M
-estimators of scatter. Rigorous statistical robustness and efficiency analysis of
MVDR beamformers based on
M
-estimators of scatter is presented in Section 2.7.
2.6.2 Subspace Methods
A standard assumption imposed by subspace methods is that the additive noise
n
is
spatially white, that is
C
(
n
)
¼ s
2
I
. We would like to stress that this assumption
does not imply that
n
is second-order circular, that is,
n
can have non-vanishing
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