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240 ANALYSIS AND PROCESSING OF RANDOM PROCESSES [CHAP 6
6.40. Find the Karhunen-Loeve expansion of the white normal (or white gaussian) noise W(t).
From Eq. (6.43),
Substituting the above expression into Eq. (6.86), we obtain
or [by Eq. (6.44)]
which indicates that all I, = o2 and &,(t) are arbitrary. Thus, any complete orthogonal set {4,(t)) with
corresponding eigenvalues A, = o2 can be used in the Karhunen-LoCve expansion of the white gaussian
noise.
FOURIER TRANSFORM OF RANDOM PROCESSES
6.41. Derive Eq. (6.94).
From Eq. (6.89),
Then
in view of Eq. (6.93).
6.42. Derive Eqs. (6.98) and (6.99).
Since X(t) is WSS, by Eq. (6.93), and letting t - s = z, we have
From the Fourier transform pair (Appendix B) 1 ++ 2nh(o), we have
Next, from Eq. (6.94) and the above result, we obtain