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Consider
the recorded data
to be the simple superposition of ``signal''
, i.e., reflection
events, and ``noise''
, i.e., multiples:
. For the special case of uncorrelated signal and noise, the so-called Wiener estimator
is a filter, which when applied to the data, yields an optimal (least-squares sense)
estimate of the embedded signal Castleman (1996). The frequency response
of this filter is
| ![\begin{displaymath}
\bf H = \frac{ P_s }{ P_n + P_s },
\end{displaymath}](img6.gif) |
(1) |
where
and
are the signal and noise power spectra, respectively.
Abma (1995) and Claerbout (1999) solved a constrained least squares problem
to separate signal from spatially uncorrelated noise:
| ![\begin{eqnarray}
\bf Nn &\approx& 0 \nonumber \\ \bf \epsilon Ss &\approx& 0
\\ \mbox{subject to} &\leftrightarrow& \bf d = s+n \nonumber
\end{eqnarray}](img9.gif) |
|
| (2) |
| |
where the operators
and
represent t-x domain convolution with
non-stationary PEF which whiten the unknown noise
and
signal
, respectively,
and
is a Lagrange multiplier. Minimizing
the quadratic
objective function suggested by equation (2) with respect to
leads to the
following expression for the estimated signal:
| ![\begin{displaymath}
\bf \hat{s} = \left( \bold N^T \bold N + \epsilon^2 \bold S^T \bold S \right)^{-1} \bold N^T \bold N \ \bold d
\end{displaymath}](img13.gif) |
(3) |
By construction, the frequency response of a PEF approximates the inverse power spectrum of
the data from which it was estimated.
Thus, we see that the approach of equation (2) is similar to the Wiener reconstruction
process.
Spitz (1999) showed that for uncorrelated signal and noise, the
signal
can be expressed in terms of a PEF,
, estimated from the data
, and a PEF,
, estimated from the noise model:
| ![\begin{displaymath}
\bold S = \bold D \bold N^{-1} .
\end{displaymath}](img15.gif) |
(4) |
Spitz' result applies to one-dimensional PEF's in the f-x domain, but our use
of the helix transform Claerbout (1998) permits stable inverse filtering
with multidimensional t-x domain filters.
Substituting
and applying the constraint
to equation (2) gives
| ![\begin{eqnarray}
\bf Ns &\approx& \bf Nd \nonumber \\ \epsilon \bold D \bold N^{-1}\bf s &\approx& \bf 0.
\end{eqnarray}](img17.gif) |
|
| (5) |
Iterative solutions to least-squares problems converge faster if the data and the model
being estimated are both uncorrelated. To precondition this problem, we again
appeal to
the Helix transform to make the change of variables
or
and apply it to equation (5):
| ![\begin{eqnarray}
{\bf NND}^{-1}\bf x &\approx& \bf Nd \nonumber \\ \epsilon \bf x &\approx& \bf 0
\end{eqnarray}](img20.gif) |
|
| (6) |
After solving equation (6) for the preconditioned solution
, we obtain
the estimated signal by reversing the change of variables:
.
Next: Filter estimation
Up: METHODOLOGY
Previous: METHODOLOGY
Stanford Exploration Project
4/27/2000