1887
Volume 56, Issue 3
  • E-ISSN: 1365-2478

Abstract

ABSTRACT

The receiver function method was originally developed to analyse earthquake data recorded by multicomponent (3C) sensors and consists in deconvolving the horizontal component by the vertical component. The deconvolution process removes travel path effects from the source to the base of the target as well as the earthquake source signature. In addition, it provides the possibility of separating the emergent P and PS waves based on adaptive subtraction between recorded components if plane waves of constant ray parameters are considered. The resulting receiver function signal is the local PS wave's impulse response generated at impedance contrasts below the 3C receiver.We propose to adapt this technique to the wide‐angle multi‐component reflection acquisition geometry. We focus on the simplest case of land data reflection acquisition. Our adapted version of the receiver function approach consists in a multi‐step procedure that first removes the P wavefield recorded on the horizontal component and next removes the source signature. The separation step is performed in the τ− domain while the source designature can be achieved in either the τ− or the domain. Our technique does not require any knowledge of the subsurface. The resulting receiver function is a pure PS‐wave reflectivity response, which can be used for amplitude versus slowness or offset analysis. Stack of the receiver function leads to a high‐quality S wave image.

Loading

Article metrics loading...

/content/journals/10.1111/j.1365-2478.2007.00685.x
2008-04-21
2024-04-25
Loading full text...

Full text loading...

References

  1. AkiK. and RichardsP.G.1980. Quantitative Seismology: Theory and Methods . W.H. Freeman and Co.
    [Google Scholar]
  2. AmmonC.J., RandallG.E. and ZandtG.1990. On the non‐uniqueness of receiver function inversions. Journal of Geophysical Research95, 15303–15318.
    [Google Scholar]
  3. AmundsenL.1999. Elimination of free surface‐related multiples without need of the source wavelet. 9th SEG meeting, Expanded Abstract.
  4. AmundsenL. and ReitanA.1995. Decomposition of multi‐component sea‐floor data into upgoing‐downgoing P and S waves. Geophysics60, 563–572.
    [Google Scholar]
  5. AtaE. and MichelenaR.J.1995. Mapping distribution of fractures in a reservoir with PS converted waves. The Leading Edge14, 644–676.
    [Google Scholar]
  6. BakerE.G., MinsterJ.B., ZandtG. and GurrolaH.1996. Constraints on crustal structure and complex Moho topography beneath Pinon Flat, California, from teleseismic receiver functions. Bulletin of the Seismological Society of America86, 1830–1844.
    [Google Scholar]
  7. BaigA.M., BostockM.G. and MercierJ.‐P.2005. Spectral reconstruction of teleseismic P Green's functions. Journal of Geophysical Research110, B08306,
    [Google Scholar]
  8. BostockM.G. and SacchiM.D.1997. Deconvolution of teleseismic recordings for mantle structure. Geophysical Journal International129, 143–152.
    [Google Scholar]
  9. CassidyJ.F.1992. Numerical experiments in brodband receiver function analysis. Bulletin of the Seismological Society of America82, 1453–1474.
    [Google Scholar]
  10. ClaytonR.W. and WigginsR.A.1976. Source shape estimation and deconvolution of teleseismic body waves. Geophysical Journal of the Royal Astronomical Society47, 151–177.
    [Google Scholar]
  11. DankbaarJ.W.M.1985. Separation of P and S waves. Geophysical Prospecting33, 970–986.
    [Google Scholar]
  12. DunneJ. and BeresfordG.1995. A review of the τ‐p transform, its implementation and its applications in seismic processing. Exploration Geophysics26, 1395–1400.
    [Google Scholar]
  13. FuchsK. and MullerG.1971. Computation of synthetic seismograms with the reflectivity method and comparison with observations. Geophysical Journals of the Royal Astronomical Society23, 417–433.
    [Google Scholar]
  14. GarottaR., GrangerP.Y. and DariuH.2002. Combined interpretation of PP and PS data provides direct access to elastic rock properties. The Leading Edge21, 532–535.
    [Google Scholar]
  15. GranliJ.R., ArntsenB., SollidA. and HildeE.1999. Imaging through gas‐filled sediments using marine shear‐wave data. Geophysics64 ( 3 ), 668–677.
    [Google Scholar]
  16. JepsenD.C. and KennettB.L.N.1990. Three component analysis of regional seismograms. Bulletin of the Seismological Society of America80, 2032–2052.
    [Google Scholar]
  17. KennettB.L.N. and KerryN.J.1979. Seismic waves in a stratified half space. Geophysical Journal of the Royal Astronomical Society57, 557–583.
    [Google Scholar]
  18. KennettB.L.N.1991. The removal of free surface interactions from three‐component seismograms. Geophysical Journal International104, 153–163.
    [Google Scholar]
  19. KikuchiM. and KanamoriH.1982. Inversion of complex body waves. Bulletin of the Seismological Society of America72, 491–506.
    [Google Scholar]
  20. KosarevG., MakeyevaL.I. and VinnikL.P.1984. Anisotropy of the mantle inferred from observations of P to S converted waves. geophysical Journal of the Royal Astronomical Society76, 209–220.
    [Google Scholar]
  21. LangstonC.A.1979. Structure under Mount Rainier, Washington, inferred from teleseismic body waves. Journal of Geophysical Research84, 4749–4762.
    [Google Scholar]
  22. LangstonC.A.1981. Evidence for the subducting lithosphere under Vancouver Island and western Oregon from teleseismic P wave conversions. Journal of Geophysical Research86, 3857–3866.
    [Google Scholar]
  23. LevinV. and ParkJ.1997. P‐SH conversions in a flat‐layered medium with anisotropy of arbitrary orientation. Geophysical Journal International131, 253–266.
    [Google Scholar]
  24. LiX.Q. and NabelekJ.L.1999. Deconvolution of teleseismic body waves for enhancing structure below a receiver array. Bulletin of the Seismological Society of America89, 190–201.
    [Google Scholar]
  25. LiX.Y.1997. Fracture reservoir delineation using multicomponent seismic data. Geophysical Prospecting45, 39–64.
    [Google Scholar]
  26. LynnH.B., SimonK.M. and BatesC.R.1996. Correlation between P‐wave AVOA and S‐wave traveltime anisotropy in a naturally fractured gas reservoir. The Leading Edge15, 931–935.
    [Google Scholar]
  27. LigorriaJ.P. and AmmonC.J.1999. Iterative deconvolution and receiver function estimation. Bulletin of the Seismological Society of America89, 19–36.
    [Google Scholar]
  28. ReadingA., KennettB.L.N. and SambridgeM.2003. Improved inversion for seismic structure using transformed S‐wavevector receiver functions: removing the effect of the free surface. Geophysical Research Letters30 ( 19 ), 1981. doi:DOI: 10.1029/2003GL018090.
    [Google Scholar]
  29. RegnierM.1988. Lateral variation of upper mantle structure beneath New caledonia determined from P‐wave receiver function; evidence for a fossil subduction zone. Geophysical Journal of the Royal Astronomical Society95, 561–577.
    [Google Scholar]
  30. RileyD.C. and ClaerboutJ.F.1976. 2‐D multiple reflections. Geophysics41, 592–620.
    [Google Scholar]
  31. SavageM.1998. Lower crustal anisotropy or dipping boundaries? Effects on receiver functions and a case study in New Zealand. Journal of Geophysical Research103, 15069–15087.
    [Google Scholar]
  32. SheehanA.F., AbersG.A., JonesC.H. and Lerner‐LamA.L.1995. Crustal thickness variations across the Colorado Rocky mountains from teleseismic receiver functions. Journal of Geophysical Research100, 391–404.
    [Google Scholar]
  33. SinghS.C., WestG.F. and ChapmanC.H.1989. On plane wave decomposition: Alias removal. Geophysics54, 1339–1343.
    [Google Scholar]
  34. TathamR.H. and McCormackM.D.1981. Multicomponent Seismology in Petroleum Exploration . SEG.
    [Google Scholar]
  35. ThomsenL.1999. Converted‐wave relection seismology over inhomogeneous anisotropic media. Geophysics64, 678–690.
    [Google Scholar]
  36. TsvankinI. and GrechkaV.2002. 3D description and inversion of reflection moveout of PS‐waves in anisotropic media. Geophysical Prospecting50, 301–316.
    [Google Scholar]
  37. VergneJ.2002. Imagerie des structures et dynamique de la lithosphere de la marge nord‐est du Tibet . PhD thesis, University of Strasbourg France.
  38. VerschuurD.J., BerkhoutA.J. and WapenaarC.P.A.1992. Adaptive surface‐related multiple elimination. Geophysics57, 1166–1177.
    [Google Scholar]
  39. VinnikL.P.1977. Detection of waves converted from P to SV in the mantle. Physics of the Earth and Planetory Interiors15, 39–45.
    [Google Scholar]
  40. VinnikL.P. and MontagnerJ.P.1996. Shear wave splitting in the mantle PS phases. Geophysical Research Letters232449–2452.
    [Google Scholar]
  41. WangY., SinghS.C. and BartonP.J.2002. Separation of P and SV wavefields from multi‐component seismic data in the τ‐p domain. Geophysical Journal International151, 663–672.
    [Google Scholar]
  42. WapenaarC.P.A, HerrmannP., VerschuurD.J. and BerkhoutA.J.1990. Decomposition of multicomponet seismic data into primary P and S wave responses. Geophysical Prospecting38, 633–661.
    [Google Scholar]
  43. YilmazO.1987. Seismic Data Processing . SEG.
    [Google Scholar]
http://instance.metastore.ingenta.com/content/journals/10.1111/j.1365-2478.2007.00685.x
Loading
/content/journals/10.1111/j.1365-2478.2007.00685.x
Loading

Data & Media 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