1887
Volume 25 Number 3
  • E-ISSN: 1365-2478

Abstract

A

Consider the mathematical model of a horizontally layered system subject to an initial downgoing source pulse in the upper layer and to the condition that no upgoing waveforms enter the layered system from below the deepest interface. The downgoing waveform (as measured from its first arrival) in each layer is necessarily minimum‐phase. The net downgoing energy in any layer, defined as the difference of the energy spectrum of the downgoing wave minus the energy spectrum of the upgoing wave, is itself in the form of an energy spectrum, that is, it is non‐negative for all frequencies. The ‐transform of the autocorrelation function corresponding to the net downgoing energy spectrum is called the net downgoing spectral function for the layer in question. The net downgoing spectral functions of any two layers and are related as follows: the product of the net downgoing spectral function of layer times the overall transmission coefficient from to equals the product of the net downgoing spectral function of layer times the overall transmission coefficient from to The net downgoing spectral function for the upper layer is called simply the spectral function of the system. In the case of a marine seismogram, the autocorrelation function corresponding to the spectral function can be used to recursively generate prediction error operators of successively increasing lengths, and at the same time the reflection coefficients at successively increasing depths. This recursive method is mathematically equivalent to that used in solving the normal equations in the case of Toeplitz forms. The upgoing wave‐form in any given layer multiplied by the direct transmission coefficient from that layer to the surface is equal to the convolution of the corresponding prediction error operator with the surface seismogram. The downgoing waveform in this given layer multiplied by the direct transmission coefficient from that layer to the surface is equal to the convolution of the corresponding hindsight error operator (i.e., the time reverse of the prediction error operator) with the surface seismogram.

Loading

Article metrics loading...

/content/journals/10.1111/j.1365-2478.1977.tb01180.x
2006-04-27
2024-04-25
Loading full text...

Full text loading...

References

  1. Anstey, N. A., 1960, Attacking the problems of the synthetic seismogram, Geoph. Prosp.8, 242–259.
    [Google Scholar]
  2. Baranov, V. and Kunetz, G., 1960, Film synthéthique avec réflexions multiples; théorie et calcul practique, Geoph. Prosp.8, 315–325.
    [Google Scholar]
  3. Bois, P., Grau, G., Hemon, C., and LaPorte, M., 1962, Calcul automatique des sismo‐grammes synthétiques en ondes planes à l'incidence normale, Rev. Inst. Français du Pétrole17, 491–522.
    [Google Scholar]
  4. Claerbout, J. F., 1968, Synthesis of a layered medium from its acoustic transmission response, Geophysics33, 264–269.
    [Google Scholar]
  5. Darby, E. K. and Neidell, N. S., 1966, Application of dynamic programming to the problem of plane wave propagation in a layered medium, Geophysics31, 1037–1048.
    [Google Scholar]
  6. Frasier, C. W., 1970, Discrete time solution of plane P‐SV waves in a plane layered medium, Geophysics35, 197–219.
    [Google Scholar]
  7. Goupillaud, P. L., 1961, An approach to inverse filtering of near surface layer effects from seismic records, Geophysics26, 754–760.
    [Google Scholar]
  8. Kunetz, G. and D'Erceville, I., 1962, Sur certaines propriétés d'une onde acoustique plane de compression dans un milieu stratifié, Annales de Géophysique18, 351–359.
    [Google Scholar]
  9. Kunetz, G., 1954, Généralisation des opérateurs d'antirésonance à nombre quelconque de réflecteurs, Geoph. Prosp.12, 283–289.
    [Google Scholar]
  10. Levinson, N., 1947, The Wiener RMS (root mean square) error criterion in filter design and prediction, JI. Math. Phys.25, 261–278.
    [Google Scholar]
  11. Riley, D. C., 1974, Wave equation synthesis and inversion of diffracted multiple seismic reflections: PhD thesis, Dept. of Geophysics, Stanford University, 101 p.
  12. Robinson, E. A., 1954, Predictive decomposition of time series with applications to seismic exploration, PhD thesis, Dept. of Geology and Geophysics, MIT, 252 p. (also published in Geophysics 32, 418–484, 1967).
  13. Robinson, E. A., 1967, Multichannel time series analysis with digital computer programs, San Francisco , Holden‐Day, Inc., 298 p.
    [Google Scholar]
  14. Robinson, E. A., 1967a, Statistical communication and detection with special reference to digital data processing of radar and seismic signals, London, Charles Griffin and Co. Ltd., and New York , Hafner Publishing Co., 362 p.
    [Google Scholar]
  15. Robinson, E. A., 1968, Basic equations for synthetic seismograms using the z‐transform approach, Geophysics33, 521–523.
    [Google Scholar]
  16. Sherwood, J. W. C. and Trorey, A. W., 1965, Minimum phase and related properties of the response of a horizontally stratified absorptive earth to plane acoustic waves, Geophysics30, 191–197.
    [Google Scholar]
  17. Treitel, S. and Robinson, E. A., 1966, Seismic wave propagation in layered media in terms of communication theory, Geophysics31, 17–32.
    [Google Scholar]
  18. Treitel, S. and Robinson, E. A., 1966a, The design of high‐resolution digital filters, IEEE Trans. on Geoscience ElectronicsGE‐4, 25–38.
    [Google Scholar]
  19. Trorey, A. W., 1962, Theoretical seismograms with frequency and depth dependent absorption, Geophysics27, 766–785.
    [Google Scholar]
  20. Wuenschel, P. C., 1960, Seismogram synthesis including multiples and transmission coefficients: Geophysics, 25, 106–129.
    [Google Scholar]
http://instance.metastore.ingenta.com/content/journals/10.1111/j.1365-2478.1977.tb01180.x
Loading
  • Article Type: Research Article

Most Cited This Month Most Cited RSS feed

This is a required field
Please enter a valid email address
Approval was a Success
Invalid data
An Error Occurred
Approval was partially successful, following selected items could not be processed due to error