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448<br />

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

Properties of Gaussian Processes<br />

Some properties of Gaussian processes are as follows:<br />

1. f x (x) depends only on C and m, which is another way of saying that the N-dimensional<br />

Gaussian PDF is completely specified by the first- and second-order moments<br />

(i.e., means, variances, and covariances).<br />

2. Since the {x i = x(t i )} are jointly Gaussian, the x i = x(t i ) are individually Gaussian.<br />

3. When C is a diagonal matrix, the random variables are uncorrelated. Furthermore, the<br />

Gaussian random variables are independent when they are uncorrelated.<br />

4. A linear transformation of a set of Gaussian random variables produces another set of<br />

Gaussian random variables.<br />

5. A wide-sense stationary Gaussian process is also strict-sense stationary † [Papoulis,<br />

1984, p. 222; Shanmugan and Breipohl, 1988, p. 141].<br />

Property 4 is very useful in the analysis of linear systems. This property, as well as the<br />

following theorem, will be proved subsequently.<br />

THEOREM. If the input to a linear system is a Gaussian random process, the system<br />

output is also a Gaussian process.<br />

Proof. The output of a linear network having an impulse response h(t) is<br />

This can be approximated by<br />

q<br />

y(t) = h(t) * x(t) = h(t - l)x(l) dl<br />

L<br />

y(t) = a<br />

N<br />

j = 1<br />

-q<br />

h(t - l j )x(l j ) ¢l<br />

which becomes exact as N gets large and ¢ → 0.<br />

The output random variables for the output random process are<br />

In matrix notation, these equations become<br />

D<br />

y 1<br />

y 2<br />

T<br />

o<br />

y N<br />

y(t 1 ) = a<br />

N<br />

o<br />

j = 1<br />

y(t 2 ) = a<br />

N<br />

j =1<br />

N<br />

y(t N ) = a [h(t N - l j ) ¢l]x(l j )<br />

j=1<br />

[h(t 1 - l j ) ¢l]x(l j )<br />

[h(t 2 - l j ) ¢l] x(l j )<br />

h 11 h 12<br />

Á h1N<br />

h 21 h 22<br />

Á h2N<br />

= D<br />

T<br />

o o ∞ o<br />

h N1 h N2<br />

Á hNN<br />

D T<br />

o<br />

x N<br />

(6–114)<br />

† This follows directly from Eq. (6–112), because the N-dimensional Gaussian PDF is a function only of t and<br />

not the absolute times.<br />

x 1<br />

x 2

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