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466<br />

Random Processes and Spectral Analysis Chap. 6<br />

The maximum (SN) out is obtained when H(f) is chosen such that equality is attained. Using<br />

Eq. (6–158), this occurs when A(f ) = KB * ( f), or<br />

which reduces to Eq. (6–155) of the theorem.<br />

From a practical viewpoint, it is realized that the constant K is arbitrary, since both the<br />

input signal and the input noise would be multiplied by K, and K cancels out when (SN) out is<br />

evaluated. However, both the output signal and the noise levels depend on the value of the<br />

constant.<br />

In this proof, no constraint was applied to assure that h(t) would be causal. Thus, the filter<br />

specified by Eq. (6–155) may not be realizable (i.e., causal). However, the transfer function<br />

given by that equation can often be approximated by a realizable (causal) filter. If the causal constraint<br />

is included (in solving for the matched filter), the problem becomes more difficult, and a<br />

linear integral equation must be solved to obtain the unknown function h(t) [Thomas, 1969].<br />

Results for White Noise<br />

H(f)2 n (f) = KS *(f)e-jvt 0<br />

For the case of white noise, the description of the matched filter is simplified as follows:<br />

For white noise, n (f) = N 0<br />

2. Thus, Eq. (6–155) becomes<br />

From this equation, we obtain the following theorem.<br />

THEOREM. When the input noise is white, the impulse response of the matched filter<br />

becomes<br />

h(t) = Cs(t 0 - t)<br />

(6–160)<br />

where C is an arbitrary real positive constant, t 0 is the time of the peak signal output,<br />

and s(t) is the known input-signal waveshape.<br />

Proof. We have<br />

h(t) = -1 [H(f)] = 2K S<br />

N * (f) e -jvt 0<br />

e jvt df<br />

0 L-q<br />

= 2K q<br />

c S(f)e j2pf(t0-t) *<br />

df d<br />

N 0 L<br />

-q<br />

= 2K<br />

N 0<br />

[s(t 0 - t)] *<br />

2 n (f)<br />

H(f) = 2K<br />

N 0<br />

S * (f)e -jvt 0<br />

But s(t) is a real signal; hence, let C = 2KN 0 , so that the impulse response is equivalent to<br />

Eq. (6–160).<br />

q

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