Digital Signal Processing Reference
In-Depth Information
where the noise variances σ q k
are ordered such that
σ q 0
σ q 1
σ q M− 1
...
(16 . 103)
Proof of Eq. (16.100). If K = M then Eq. (16.100) reduces to
M M− 1
=0
σ q
σ q 2
1 .
(16 . 104)
M− 1
=0
Now, from Cauchy-Schwartz inequality we have
σ q 2
M− 1
M− 1
M− 1
M− 1
1 2
σ q = M
σ q
=0
=0
=0
=0
which proves (16.104) indeed. Next assume that the power p 0 is such that
K<M. That is, the noise variances are such that Eqs. (16.101) and (16.102)
are true. For simplicity, we first assume that
σ q K
= σ q K +1 = ... = σ q M− 1
(16 . 105)
and that Eq. (16.101) holds with equality:
K− 1
K− 1
σ q = σ q k
p 0 +
σ q ,
K
k
M
1 .
(16 . 106)
=0
=0
Substituting into Eq. (16.100) we can rewrite it as
M σ q K K− 1
σ q
=0
K− 1
=0
σ q 2 +( M
K ) σ q K K− 1
σ q
=0
M σ q K K− 1
σ q
σ q K− 1
=0
=0
K ) σ q K 2
1 ,
K− 1
=0
σ q +( M
which simplifies to
M σ q K K− 1
σ q
σ q K− 1
q K
=0
=0
K− 1
=0
σ q +( M
K ) σ q K
K ) σ q K 2 1 .
K− 1
=0
σ q +( M
This can be rewritten as
K ) σ q K + M K− 1
σ q
M ( M
=0
K ) σ q K 2
1 ,
K− 1
=0
σ q +( M
 
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