MAXIMUM LIKELIHOOD FILTERING OF REFLECTION SEISMOGRAPH DATA

Geophysics ◽  
1978 ◽  
Vol 43 (3) ◽  
pp. 497-513 ◽  
Author(s):  
Edward Mercado

Two types of adaptive multichannel filters applied to exploration reflection seismograph data are the maximum likelihood filter and the Wiener filter. Derived equations for the two types of filters demonstrate that the maximum likelihood filter equations are identical in form to the Wiener equations and are solved by the same matrix inversion techniques. Application of the maximum likelihood filter to common‐depth‐point (CDP) data demonstrates that the output reflection quality is sensitive to reflection alignment on input traces. Presently, sufficient coherency of reflections on input traces can be achieved only on CDP traces with a time window in which the reflection signal is dominant or on vertical array data for which reflection alignment is straight‐forward.

1990 ◽  
Vol 80 (6B) ◽  
pp. 1934-1950 ◽  
Author(s):  
A. F. Kushnir ◽  
V. M. Lapshin ◽  
V. I. Pinsky ◽  
J. Fyen

Abstract A generalization of Capon's maximum-likelihood technique for detection and estimation of seismic signals is introduced. By using a multi-dimensional autoregressive approximation of seismic array noise, we have developed a technique to use Capon's multi-channel filter for on-line processing. Such autoregressive adaptation to the curent noise matrix power spectrum is shown to yield good suppression of mutually correlated array noise processes. As an example, this technique is applied to detection of a small Semipalatinsk underground explosion recorded at the ARCESS array.


2012 ◽  
Vol 131 (4) ◽  
pp. 3488-3488
Author(s):  
Xinmin Ren ◽  
Guofeng Zheng ◽  
Qihu LI ◽  
Guiqing Sun ◽  
Haining Huang ◽  
...  

2011 ◽  
Vol 101 (6) ◽  
pp. 2887-2896 ◽  
Author(s):  
J. Wang ◽  
J. Schweitzer ◽  
F. Tilmann ◽  
R. S. White ◽  
H. Soosalu

2020 ◽  
Vol 1 ◽  
pp. 168
Author(s):  
J. C. Varvitsiotis ◽  
L. D. Skouras

Using matrix-inversion techniques effective interactions for the sd and ρ shells are determined in the complete space 0hω + 2hω. The derived interactions are used to determine the spectra of A =18-20 and A=5-15 nuclei and compare them with experiment.


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