TY - JOUR
T1 - P-wave anisotropic tomography beneath Northeast Japan
AU - Wang, Jian
AU - Zhao, Dapeng
N1 - Funding Information:
We thank the data centers of Hi-net, Tohoku University and JMA seismic networks for providing the high-quality P-wave arrival time data used in this study. This work was supported by a research grant (Kiban-A 17204037) from the Japanese Ministry of Education and Science to D. Zhao. We thank Dr. J. Nakajima for providing the shear-wave splitting data as shown in Fig. 14 . We are indebted to G. Jiang, S. Xia, Y. Tian, S. Gupta and S. Padhy for thoughtful discussions. Figures are prepared with GMT software ( Wessel and Smith, 1995 ). Prof. G. Helffrich (the editor) and two anonymous referees provided thoughtful review comments that improved the manuscript.
PY - 2008/9
Y1 - 2008/9
N2 - We determined a 3-D P-wave anisotropic tomography beneath Northeast Japan by using first P-arrival times. The travel-time inversion is parameterized with an isotropic component and two anisotropic parameters for each grid node by assuming P-wave azimuthal anisotropy with hexagonal symmetry axis distributed horizontally. The geometries of the Conrad and Moho discontinuities and the upper boundary of the subducting Pacific plate are taken into account in the model. Our extensive synthetic tests show that the anisotropic velocity inversion method is reliable. Our results show that low-velocity zones exist below active volcanoes in the crust, in the fore-arc mantle wedge and in the central portion of the mantle wedge above the high-velocity Pacific slab, which are similar to the previous tomographic images. Anisotropic velocity variations are revealed in the crust, mantle wedge and the subducting Pacific slab. The anisotropic patterns are complex and different in the upper and lower crust. In the mantle wedge, the fast direction of P-velocity is generally trench-parallel in the fore-arc area, while it becomes trench-normal in the back-arc area, which agree well with the shear-wave splitting results. The trench-parallel fast direction is revealed beneath the volcanic front, which may suggest the existence of complex 3-D mantle flows in the mantle wedge. The fast-velocity direction in the subducting Pacific slab is mostly N-S, which is likely due to the original fossil anisotropy of the Pacific plate formed at the mid-ocean ridge. Our result also suggests that the anisotropy is weak in the upper crust and the average amplitude of the velocity anisotropy in the mantle is no larger than 4%.
AB - We determined a 3-D P-wave anisotropic tomography beneath Northeast Japan by using first P-arrival times. The travel-time inversion is parameterized with an isotropic component and two anisotropic parameters for each grid node by assuming P-wave azimuthal anisotropy with hexagonal symmetry axis distributed horizontally. The geometries of the Conrad and Moho discontinuities and the upper boundary of the subducting Pacific plate are taken into account in the model. Our extensive synthetic tests show that the anisotropic velocity inversion method is reliable. Our results show that low-velocity zones exist below active volcanoes in the crust, in the fore-arc mantle wedge and in the central portion of the mantle wedge above the high-velocity Pacific slab, which are similar to the previous tomographic images. Anisotropic velocity variations are revealed in the crust, mantle wedge and the subducting Pacific slab. The anisotropic patterns are complex and different in the upper and lower crust. In the mantle wedge, the fast direction of P-velocity is generally trench-parallel in the fore-arc area, while it becomes trench-normal in the back-arc area, which agree well with the shear-wave splitting results. The trench-parallel fast direction is revealed beneath the volcanic front, which may suggest the existence of complex 3-D mantle flows in the mantle wedge. The fast-velocity direction in the subducting Pacific slab is mostly N-S, which is likely due to the original fossil anisotropy of the Pacific plate formed at the mid-ocean ridge. Our result also suggests that the anisotropy is weak in the upper crust and the average amplitude of the velocity anisotropy in the mantle is no larger than 4%.
KW - Anisotropic tomography
KW - Hexagonal symmetry axis
KW - Northeast Japan
KW - P-wave azimuthal anisotropy
KW - Subducting Pacific slab
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U2 - 10.1016/j.pepi.2008.07.042
DO - 10.1016/j.pepi.2008.07.042
M3 - Article
AN - SCOPUS:53249105314
SN - 0031-9201
VL - 170
SP - 115
EP - 133
JO - Physics of the Earth and Planetary Interiors
JF - Physics of the Earth and Planetary Interiors
IS - 1-2
ER -