Imaging Offsets in the Moho: Synthetic Tests using Gaussian Beams with Teleseismic Waves

We carry out a sequence of numerical tests to understand conditions under which rapid changes in crustal thickness can be reliably imaged by teleseismic body waves. Using the finite-difference method over a 2-D grid, we compute synthetic seismograms resulting from a planar P-wavefield incident below the grid. We then image the Moho using a migration scheme based on the Gaussian beam representation of the wavefield. The use of Gaussian beams for the downward propagation of the wavefield is particularly advantageous in certain geologically critical cases such as overthrusting of continental lithosphere, resulting in the juxtaposition of high-velocity mantle material over crustal rocks. In contrast to ray-based methods, Gaussian beam migration requires no special treatment to handle such heterogeneities. Our results suggest that with adequate station spacing and signal-to-noise ratios, offsets of the Moho, on the order of 10 km in height, can be reliably imaged beneath thickened crust at depths of about 50 km. Furthermore, even sharp corners and edges are faithfully imaged when precise values of seismic wave speeds are available. Our tests also demonstrate that flexibility in choices of different types of seismic phases is important, because any single phase has trade-offs in issues such as spatial resolution, array aperture, and amplitude of signals.

[1]  P. Davy,et al.  Shortening of analogue models of the continental lithosphere: New hypothesis for the formation of the Tibetan plateau , 1994 .

[2]  S. Scarascia,et al.  Crustal structures in the central-eastern Alpine sector: A revision of the available DSS data , 1997 .

[3]  A. Hirn,et al.  Crustal structure and variability of the Himalayan border of Tibet , 1984, Nature.

[4]  L. Amundsen,et al.  Introduction to Petroleum Seismology , 2005 .

[5]  J. Nábělek,et al.  Deconvolution of teleseismic body waves for enhancing structure beneath a seismometer array , 1999, Bulletin of the Seismological Society of America.

[6]  M. McNutt,et al.  Lithospheric deformation beneath the Altyn Tagh and West Kunlun faults from recent gravity surveys , 2004 .

[7]  P. Schultz,et al.  Fundamentals of geophysical data processing , 1979 .

[8]  H. M. Iyer,et al.  Seismic tomography : theory and practice , 1993 .

[9]  Kamal M. Al-Yahya,et al.  Velocity analysis by iterative profile migration , 1987 .

[10]  M. M. Popov,et al.  Computation of wave fields in inhomogeneous media — Gaussian beam approach , 1982 .

[11]  Michael G. Bostock,et al.  Migration of scattered teleseismic body waves , 1999 .

[12]  Michael G. Bostock,et al.  Multiparameter two-dimensional inversion of scattered teleseismic body waves 1. Theory for oblique incidence , 2001 .

[13]  T. Tseng,et al.  Probing the Southern Indian Shield with P-Wave Receiver-Function Profiles , 2006 .

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

[15]  Zhu,et al.  Moho offset across the northern margin of the tibetan plateau , 1998, Science.

[16]  Wang-Ping Chen,et al.  Earthquakes Beneath the Himalayas and Tibet: Evidence for Strong Lithospheric Mantle , 2004, Science.

[17]  J. Sheng,et al.  Correlation Migration Using Gaussian Beams of Scattered Teleseismic Body Waves , 2006 .

[18]  V. Červený,et al.  Gaussian beam synthetic seismograms , 1985 .

[19]  N. R. Hill,et al.  Prestack Gaussian‐beam depth migration , 2001 .

[20]  Norman Bleistein,et al.  Migration velocity analysis; theory and an iterative algorithm , 1995 .

[21]  Robert L. Nowack,et al.  Calculation of Synthetic Seismograms with Gaussian Beams , 2003 .

[22]  Robert L. Nowack,et al.  Gaussian beam synthetic seismograms , 1986 .

[23]  G. Randall,et al.  On the nonuniqueness of receiver function inversions , 1990 .

[24]  Mei Jiang,et al.  Teleseismic imaging of subducting lithosphere and Moho offsets beneath western Tibet , 2004 .

[25]  K. Fuchs,et al.  Composition, structure, and dynamics of the lithosphere-asthenosphere system , 1987 .

[26]  J. Virieux P-SV wave propagation in heterogeneous media: Velocity‐stress finite‐difference method , 1986 .

[27]  B. Goleby,et al.  Basement and Cover Thrust Tectonics in Central Australia Based on the Arunta-Amadeus Seismic-Reflection Profile , 1992 .

[28]  T. Minshull,et al.  Evolution of magma-poor continental margins from rifting to seafloor spreading , 2001, Nature.

[29]  N. R. Hill,et al.  Gaussian beam migration , 1990 .