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  4. Anisotropy in the oceanic lithosphere from the study of local intraplate earthquakes on the west flank of the southern East Pacific Rise: Shear wave splitting and waveform modeling
 
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Anisotropy in the oceanic lithosphere from the study of local intraplate earthquakes on the west flank of the southern East Pacific Rise: Shear wave splitting and waveform modeling

Journal
Journal of Geophysical Research: Solid Earth
Journal Volume
104
Journal Issue
B5
Date Issued
1999-05-10
Author(s)
SHU-HUEI HUNG  
Forsyth, Donald W.
DOI
10.1029/1999JB900046
URI
https://scholars.lib.ntu.edu.tw/handle/123456789/412267
URL
https://api.elsevier.com/content/abstract/scopus_id/0033542006
Abstract
Shear wave splitting is observed on ocean bottom seismometer records from local, intraplate microearthquakes on the west flank of the East Pacific Rise at 18°S. Split times reach a maximum of about 0.2 s. For most of the incoming waves with long mantle paths (∼20 km), the polarization direction of the fast arrival is subparallel to the spreading direction, which we attribute to anisotropy caused by the strain-induced preferential orientation of olivine. In contrast, for some records with short paths or shallower sources or propagation along the spreading direction, the fast direction is nearly parallel to the ridge axis. These polarizations are probably caused by seismic anisotropy from aligned cracks in the uppermost crust. In addition, for some events, the apparent splitting is frequency dependent. To explore the pattern of shear wave splitting that would be expected for nonvertical paths in an oceanic lithosphere with two distinct anisotropic layers, we generate synthetic seismograms for a variety of source depths and mechanisms. We employ a multidomain, pseudospectral method to simulate the elastic wave fields from point sources in an inhomogeneous, anisotropic medium. Splitting parameters measured from synthetic S waves demonstrate that the apparent fast direction is not always parallel to the symmetry axes and that, in some cases, fast directions at higher frequencies will be more characteristic of the shallower crustal anisotropy while fast directions at lower frequencies are dominated by the mantle portion of the path. Most of the observed characteristics of splitting can be reproduced if there is approximately 8% S wave anisotropy in the mantle and an average of about 6% S wave anisotropy in the upper crustal, seismic layer 2. Copyright 1999 by the American Geophysical Union.
Type
journal article

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