Digital Signal Processing Reference
In-Depth Information
Thus, insertion of the unitary matrices does not affect the zero-forcing property,
the transmitted power, or the average MSE. For example, if
{ F , G }
is an MMSE
{ FU , UG }
transceiver, then so is the modified transceiver
. Although U does
not change the MSE, we will see that we can reduce the average error probability
(16.7) by optimizing U .
16.2.2 Minimizing error probability by optimizing U
The average symbol error probability in Fig. 16.2 is, from Eq. (16.7),
A
E s,k
,
M− 1
c
M
P e ( y )=
Q
(16 . 14)
k =0
where the argument vector y is defined as
y =[
E s, 0
E s, 1
...
E s,M− 1 ] .
(16 . 15)
( A/ y )isa convex function of y
as long as the signal-to-error ratio exceeds a certain threshold. This idea was
also discussed in Chap. 11 (Sec. 11.5). More precisely
It is shown in Sec. 21.2.3 of Chap. 21 that
Q
is convex in
A
E s,k
E s,k <A 2 / 3
E s,k
for
Q
(16 . 16)
E s,k >A 2 / 3 .
concave in
E s,k
for
Assuming that the errors
E s,k are su ciently small, the convexity condition
holds. In Sec. 11.5 of Chap. 11 we presented examples of typical signal-to-
noise ratios for which convexity holds, and found that the assumption is often
reasonable.
Assuming the convexity condition holds, we conclude from Chap. 21 (Sec.
21.4) that
P y ( y ) in Eq. (16.14) is a Schur-convex function of y . By definition,
what this means is that, if a vector y 1
is majorized by y 2
(for definitions see
Sec. 21.3, Chap. 21), then
≤P e ( y 2 ) . (16 . 17)
Now refer to Eq. (16.10). The freedom to change the unitary matrix U gives
us the freedom to adjust the elements [ E s ] kk , but only subject to the constraint
that their sum be constant (from Eq. (16.12)). We now use a result from Chap.
21 (Lemma 21.1) which says that the vector
P e ( y 1 )
α [1
1
...
1] ,
α> 0 ,
is majorized by any vector of the form
0 ,
with identical sum, that is, k y k = αM. Thus the unitary U that minimizes
P e ( y ) is the one that equalizes the diagonal elements of E s ,thatis,
[ y 0
y 1
...
y M− 1 ] ,
k
1
×
...
×
×
1
...
×
UE x U = α
= E s .
(16 . 18)
.
.
.
. . .
××
...
1
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