Seismic anisotropy from local earthquakes in the transition region from a subduction to a strike-slip plate boundary, New Zealand

Citation
E. Audoine et al., Seismic anisotropy from local earthquakes in the transition region from a subduction to a strike-slip plate boundary, New Zealand, J GEO R-SOL, 105(B4), 2000, pp. 8013-8033
Citations number
52
Categorie Soggetti
Earth Sciences
Journal title
JOURNAL OF GEOPHYSICAL RESEARCH-SOLID EARTH
ISSN journal
21699313 → ACNP
Volume
105
Issue
B4
Year of publication
2000
Pages
8013 - 8033
Database
ISI
SICI code
0148-0227(20000410)105:B4<8013:SAFLEI>2.0.ZU;2-Z
Abstract
Shear wave splitting is used to investigate anisotropy in the crust and upp er mantle in a subduction zone (lower half of the North Island of New Zeala nd), and its transition to oblique transform faulting (Marlborough area, no rthern South Island). In Marlborough, delay times show almost no increase w ith depth, and it is most likely that the higher frequency phases used in t his study respond mainly to lithospheric anisotropy. In the central Marlbor ough Fault System (MFS), fast polarizations are subparallel to the faults. Anisotropy is attributed to the presence of metamorphosed schist (eclogite) , of 30 +/- 10 km thickness and located 50-80 km beneath the MFS. On the ed ges of the MFS, fast polarizations are parallel to the maximum compressive stress direction, consistent with crack-induced anisotropy in the crust. Th e shear zone, which is as wide as the island in the mantle as inferred from SKS phases, seems to occur in a narrower zone in the crust. In the lower h alf of the North Island, fast polarizations from events at all depths are o riented parallel to the strike of the Hikurangi subduction zone as well as to the faults. Polarisations are similar to those of SKS phases, which main ly sample the mantle. This suggests that the lithosphere and the upper mant le asthenosphere deform in a coherent strike-slip shear. We calculate 1.2 /- 0.3% velocity anisotropy in the first 200 km of the mantle from increasi ng delay times with depth. In order to match the SKS delay times, this resu lt requires the presence of anisotropic material down to 580 +/- 100-km dep th, or a change in anisotropy with depth, or frequency dependent splitting.