Probability, Random Variables, and Random Processes: Theory and Signal Processing Applications
by John J. Shynk
8.4 EIGENFUNCTIONS OF RXX(τ)
Consider the integral equation for the Karhunen-Loève expansion (KLE) in (7.258), but with the finite limits [0, T] extended to
:
where
are eigenfunctions and {λ n} are eigenvalues. Since X(t) is wide-sense stationary, the argument of the autocorrelation function depends on the difference of the two time instants. As a result, this integral has the form of a convolution, corresponding to the LTI system in Figure 8.1, given by
(8.55)
For an LTI system, complex exponentials are eigenfunctions:
(8.56)
where we have changed variables to v = t−τ, and
(8.57)
is the frequency response of h(t) evaluated at the particular frequency ω n. This is a fundamental result covered in basic courses on signals and systems: the output has the same frequency as the input, and only its magnitude and phase are possibly different, as determined by H(ω n). Since the autocorrelation ...
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