Fresnel volume migration of multicomponent data

If the aperture of a seismic reflection experiment is strongly limited, Kirchhoff migration suffers from strong artifacts attributable to incomplete summation. This can be overcome by restricting the migration operator to the region that physically contributes to a reflection event. Examples of such limited-aperture experiments include data acquisition in boreholes, tunnels, and mines. We present an extension to three-component (3C) Kirchhoff prestack depth migration, where the migration operator is restricted to the Fresnel volume of the specular reflected raypath. We use the measured polarization direction at a 3C receiver to determine points of specular reflection. In homogeneous media, the polarization angle of 3C data can be used directly to decide whether a certain image point belongs to the Fresnel volume of a specular reflection. In heterogeneous media, the Fresnel volume around an image point is approximated by means of paraxial ray tracing. The method is tested on a synthetic vertical seismic profiling experiment with strongly limited aperture. Migration artifacts and crosstalk effects from converted waves are strongly reduced compared with standard migration schemes. The method is successfully applied to seismic data acquired in a tunnel.

[1]  Jörg Schleicher,et al.  Aperture effects in 2.5D Kirchhoff migration: A geometrical explanation , 2003 .

[2]  Jianguo Sun,et al.  Limited‐aperture migration , 2000 .

[3]  H. Gebrande,et al.  Focusing in Prestack Isochrone Migration Using Instantaneous Slowness Information , 1999 .

[4]  R. James Brown,et al.  Converted-wave seismic exploration: Methods , 2002 .

[5]  Gerard T. Schuster,et al.  2-D wavepath migration , 2001 .

[6]  Yuzuru Ashida,et al.  Seismic imaging ahead of tunnel face with three component geophones , 2002 .

[7]  G. Kneib,et al.  Automatic seismic prediction ahead of the tunnel boring machine , 2000 .

[8]  V. Červený,et al.  Seismic Ray Theory , 2001, Encyclopedia of Solid Earth Geophysics.

[9]  P. Earle POLARIZATION OF THE EARTH'S TELESEISMIC WAVEFIELD , 1999 .

[10]  Martin Schimmel,et al.  The use of instantaneous polarization attributes for seismic signal detection and image enhancement , 2003 .

[11]  C. Müller On the Nature of Scattering from Isolated Perturbations in Elastic Media and the Consequences for Processing of Seismic Data , 2006 .

[12]  T. Bohlen,et al.  ISIS – Integrated Seismic Imaging System for the Geological Prediction ahead of Underground Construction , 2003 .

[13]  Gerard T. Schuster,et al.  3D wavepath migration , 2003 .

[14]  E. Brückl,et al.  A study of the application of VSP to exploration ahead of a tunnel , 2001 .

[15]  D. Snyder,et al.  Downhole seismic imaging of a massive sulfide orebody with mode-converted waves, Halfmile Lake, New Brunswick, Canada , 2004 .

[16]  Vlastislav Cerveny,et al.  Seismic Ray Theory , 2003 .

[17]  Multicomponent common-receiver gather migration of single-level walk-away seismic profiles , 1991 .

[18]  Y. Kravtsov,et al.  Geometrical optics of inhomogeneous media , 2019, Geometrical Optics of Weakly Anisotropic Media.

[19]  Vlastislav Cerveny,et al.  Fresnel volume ray tracing , 1992 .

[20]  Toru Takahashi Prestack migration using arrival angle information , 1995 .

[21]  Martin Tygel,et al.  3-D true‐amplitude finite‐offset migration , 1993 .

[22]  E. R. Kanasewich,et al.  Time sequence analysis in geophysics , 1973 .

[23]  Stefan Buske,et al.  FRESNEL-VOLUME MULTICOMPONENT MIGRATION , 2003 .

[24]  S. Shapiro,et al.  Modeling the propagation of elastic waves using a modified finite-difference grid , 2000 .