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B. P. Lathi, Zhi Ding - Modern Digital and Analog Communication Systems-Oxford University Press (2009)

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10. 9 Nonwhite (Colored) Channel Noise 577

Substituting Eq. (10.128) into Eq. (10.129) and observing that the set <pi is orthonormal, we

have

(10.130)

Hence, for the same performance ( error probability), the mean energy of the simplex signal set

is l - l / M times that of the orthogonal signal set. For M » 1, the difference is not significant.

For this reason and because of the simplicity in generating, orthogonal signals, rather than

simplex signals are used in practice whenever M exceeds 4 or 5.

Tn Sec. 13.6, we shall show that in the limit as M -+ oo, the orthogonal (as well as the

simplex) signals attain the upper bound of performance predicted by Shannon's theorem.

10. 9 NONWHITE (COLORED) CHANNEL NOISE

Thus far we have restricted our analysis exclusively to white Gaussian channel noise. Our

analysis can be extended to nonwhite, or colored, Gaussian channel noise. To proceed,

the Karhunen-Loeve expansion of Eq. (10.57) must be solved for the colored noise with

autocorrelation function R x (t, ti). This general solution, however, can be quite complex to

implement. 4

Fortunately, for a large class of colored Gaussian noises, the power spectral density Sn (f) is

nonzero within the message signal bandwidth B. This property provides an effective alternative.

We use a noise-whitening filter H (f) at the input of the receiver, where

H (f) = __ l_e-J2:n:ftd

Jsn (f)

The delay tc1 is introduced to ensure that the whitening filter is causal (realizable).

Consider a signal set {si (t)} and a channel noise n(t) that is not white [Sn (f) is not constant].

At the input of the receiver, we use a noise-whitening filter H (f) that transforms the colored

noise into white noise (Fig. 10.34). But it also alters the signal set {si (t)} to {s;(t)}, where

s; (t) = s;(t) * h(t)

We now have a new signal set {s; (t)} mixed with white Gaussian noise, for which the optimum

receiver and the corresponding error probability can be determined by the method discussed

earlier.

Figure 10.34

Optimum Mary

receiver for

nonwhite

channel noise.

n(I)

/s1 (t) ) !

Noise-whitening Optimum receiver

filter

for

S; (t) + H(f)

{s';

n(t)

s '; (t) + n,Jt)

(t) }in white noise

Decision

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