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Kolmogorov 1939 spectral factorization provides a highly
efficient Fourier method for calculating a minimum phase time domain
function with a given power spectrum. The Kolmogorov spectral
factorization method is commonly referred to as the Hilbert transform
method within the signal processing community
[e.g. Robinson and Treitel (1980)],
although they are equivalent.
Following Claerbout 1992,
we will describe the method briefly with Z transform notation.
In this notation, is the unit delay
operator, and functions can be evaluated either in the frequency
domain as functions of , or in the time domain as the
coefficients of the polynomial in Z.
Causal functions can, therefore, be written as polynomials with
non-negative powers of Z, whereas anti-causal functions contain
non-positive powers of Z.
The spectral factorization problem can be summarized as given a power
spectrum, S(Z), we must find a minimum phase function such that
| |
(3) |
Since S(Z) is a power spectrum, it is non-negative by definition for
all ; however, the Kolmogorov process places the additional
requirement that S(Z) contains no zeros. If this is the case, then we
can safely take its logarithm,
| |
(4) |
Since is real and even, its time domain representation is
also real and even. We can therefore isolate its causal part,
C(Z), and its anti-causal part, :
| |
(5) |
Once we have C(Z), we can easily obtain B(Z) through
| |
(6) |
To verify that B(Z) of this form does indeed satisfy
equation (), consider
| |
(7) |
| (8) |
| (9) |
| (10) |
B(Z) will be causal since C(Z) was causal, and a power series
expansion proves that the exponential of a causal function is also
causal. It is also clear that 1/B(Z)=e-C(Z) will also be causal
in the time domain. Therefore, B(Z) will be causal, and will have a
causal inverse. Hence B(Z) satisfies the definition of minimum phase
given above.
Next: Multi-dimensional factorization
Up: Model of stochastic oscillations
Previous: Model of stochastic oscillations
Stanford Exploration Project
5/27/2001