Page 243 - Global Tectonics
P. 243

CONTINENTAL TRANSFORMS AND STRIKE-SLIP FAULTS  229



            the Canterbury Plain to a maximum depth of 37 km   Below the crustal root, teleseismic data show that
            below a point located 45 km southeast of the surface   deformation becomes progressively wider with depth.
            trace of the Alpine Fault. The root is asymmetric and   Measurements of P n  wave speeds (Scherwath  et al.,

            mimics the tapered profile of the Southern Alps at the   2002; Baldock & Stern, 2005) and shear wave (SKS) split-
            surface: Moho depths southeast of the fault decrease   ting (Klosko et al., 1999; Duclos et al., 2005) suggest the
            more gradually than those on its northwest side   presence of a zone of distributed ductile deformation
            (Scherwath et al., 2003; Henrys et al., 2004). The root is   in the upper mantle beneath the Alpine Fault. Fast
            composed mostly of thickened upper crust with seismic   polarization directions generally are oriented subparal-
                                              −1
            velocities ranging between 5.7 and 6.2 km s  (Scher-  lel to the fault strike (Fig. 8.15), suggesting fl ow parallel
            wath et al., 2003; Van Avendonk et al., 2004). At large   to the plate boundary. Baldock & Stern (2005) found
            distances from the plate boundary, the upper crust   evidence for two distinctive domains beneath the South
            shows a normal thickness of ∼15 km. A thin (3–5 km)   Island: a 335-km-wide zone of mantle deformation in
                                                    −1
            lower crust with a velocity range of 6.5–7.1 km s    the south and a narrower, ∼200-km-wide zone in the
            occurs at the base of the root. A low velocity zone   north (Fig. 8.15). These widths and the orientation of
            occurs in the middle and lower crust below the fault   the mantle anisotropy are consistent with a model of
            trace, most likely as a result of high fl uid  pressure   transpression involving 800  ± 200 km of right lateral
            (Section 8.6.3) (Stern  et al., 2001, 2002), and extends   strike-slip displacement, which is close to that predicted
            downward into the upper mantle.              by geologic reconstructions.


                                166° E                168°  42°            170°   40°    171° E




                                                                                   N
                                         Western limit to deformation
                                             +
                                          11.5   2.4%                                 40° S
                                              -
                                                                                       173° E


                                                                       AF
                                                        k


                                                                                       175° E


                                                               T3
                                             +
                                          6.5   2.5%    0   3%                        42° S
                                                         +
                                             -
                                                         -
                          Eastern limit to deformation    T1            100 km
                                           T2

            Figure 8.15  Map showing the geometry of the SIGHT experiment and SKS measurements with an interpretation of
            mantle deformation below the Alpine Fault (AF) (image provided by T. Stern and modified from Baldock & Stern, 2005, with

            permission from the Geological Society of America). Three seismic transects (T1, T2, T3) are shown. Black bars indicate
            direction of maximum seismic velocity. Bar length is proportional to the amplitude of shear wave splitting determined
            from the SKS results of Klosko et al. (1999). P n  anisotropy measurement of 11.5 ± 2.4% is from Scherwath et al. (2002).
   238   239   240   241   242   243   244   245   246   247   248