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Inversion of Scholte wave dispersion and waveform modeling for shallow structure of the Ninetyeast Ridge
Authors:Xuan Nhi Nguyen  Torsten Dahm  Ingo Grevemeyer
Institution:1. Institut für Geophysik, Universit?t Hamburg, Bundesstrasse 55, 20146, Hamburg, Germany
2. Institut für Geophysik, Technische Universit?t Bergakademie Freiberg, Gustav-Zeuner-Stra?e 12, 09599, Freiberg, Germany
3. IFM–GEOMAR, Leibniz Institut für Marine Geowissenschaften, Wischhofstrasse 1-3, 24148, Kiel, Germany
Abstract:The construction of S-wave velocity models of marine sediments down to hundreds of meters below the seafloor is important in a number of disciplines. One of the most significant trends in marine geophysics is to use interface waves to estimate shallow shear velocities which play an important role in determining the shallow crustal structure. In marine settings, the waves trapped near the fluid–solid interface are called Scholte waves, and this is the subject of the study. In 1998, there were experiments on the Ninetyeast Ridge (Central Indian Ocean) to study the shallow seismic structure at the drilled site. The data were acquired by both ocean bottom seismometer and ocean bottom hydrophone. A new type of seafloor implosion sources has been used in this experiment, which successfully excited fast and high frequency (>500 Hz) body waves and slow, intermediate frequency (<20 Hz) Scholte waves. The fundamental and first higher mode Scholte waves have both been excited by the implosion source. Here, the Scholte waves are investigated with a full waveform modeling and a group velocity inversion approach. Shear wave velocities for the uppermost layers of the region are inferred and results from the different methods are compared. We find that the full waveform modeling is important to understand the intrinsic attenuation of the Scholte waves between 1 and 20 Hz. The modeling shows that the S-wave velocity varies from 195 to 350 m/s in the first 16 m of the uppermost layer. Depths levels of high S-wave impedance contrasts compare well to the layer depth derived from a P-wave analysis as well as from drilling data. As expected, the P- to S-wave velocity ratio is very high in the uppermost 16 m of the seafloor and the Poisson ratio is nearly 0.5. Depth levels of high S-wave impedance contrasts are comparable to the layer depth derived from drilling data.
Keywords:Scholte wave  Sediments  Seismic waves  Shear deformation  Velocity measurement  Seafloor phenomena  Waveform modeling  Dispersion (waves)  Sensitivity kernel  Implosive source
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