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OROGENIC BELTS  289



               In the Andes, compressional regimes have been   to bending and other mechanical adjustments within
            established several times since the early Mesozoic, with   the subducting oceanic lithosphere. Farther east thrust-
            the most recent phase beginning about 25–30 Ma   type solutions are most abundant with some strike-slip
            (Allmendinger et al., 1997). The beginning of this latest   motion (Gutscher  et al., 2000; Siame  et al., 2005). In
            phase of compression has been interpreted to refl ect   general, the axes of maximum compressional stress
            two major processes: the trenchward acceleration of   are aligned with the plate motion vector, suggesting
            the South American plate (Pardo-Casas & Molnar, 1987;   that plate boundary stresses are transmitted up to
            DeMets  et al., 1990; Somoza, 1998) and strong inter-  several hundred kilometers into the South American
            plate coupling between the subducting oceanic litho-  plate.
            sphere and the overriding continent (Jordan et al., 1983;   The distribution of earthquake hypocenters with
            Gutscher et al., 2000; Yáñez & Cembrano, 2004). One   depth indicates that the margin is divided into fl at and
            of the principal aims of tectonic studies in the Andes is   steep subduction segments (Barazangi & Isacks, 1979;
            to determine the origin of the highly variable response   Jordan et al., 1983). Beneath southern Peru and Bolivia,
            of the South American plate to this compression. This   the Benioff zone dips about 30° (Fig. 10.3a,b). Beneath
            section provides a discussion of the fi rst-order physical   north-central Chile, it initially forms an angle of 30° to
            characteristics of the central and southern Andes that   a depth of ∼100 km and then dips at angles of 0–10° for
            allow geoscientists to make inferences about the genesis   several hundred kilometers (Fig. 10.3c). To allow sub-
            of the mountain range.                       duction to take place at such different angles, either a
                                                         lithospheric tear or a highly distorted down-going plate
                                                         must accommodate the transitions between the fl at and
                                                         steep segments.
                                                            Above zones of flat subduction, shallow seismicity

            10.2.2 Seismicity,                           is more abundant and broadly distributed than over
            plate motions, and                           neighboring steep segments (Barazangi & Isacks, 1979;
                                                         Jordan et al., 1983). The seismic energy released in the
            subduction geometry                          upper plate above flat slabs is, on average, three to fi ve

                                                         times greater than in steep (>30°) segments between
            The general pattern of seismicity in the Andes is in   250 and 800 km from the trench (Gutscher et al., 2000).
            accord with the eastward subduction of the Nazca plate   These differences suggest that flat slab segments are

            beneath South America (Molnar & Chen, 1982). Geo-  strongly coupled to the overlying continental plate
            detic data suggest that convergence velocities with   (Section 9.6). The coupling appears to be controlled by
                                          −1
            respect to South America are 66–74 mm a  at the trench   the presence of a cool slab at shallow depths beneath
            (Norabuena et al., 1998; Angermann et al., 1999; Sella   the continental lithosphere, which strengthens the
                                                    −1
            et al., 2002). These rates are slower than the 77–80 mm a    upper plate and enables it to transmit stresses over long
            predicted by the NUVEL-1A model of plate motions   distances.


            (Section 5.8) and appear to reflect a deceleration from   In addition to influencing mechanical behavior,
                                −1
            a peak of some 150 mm a  at 25 Ma (Pardo-Casas &   variations in the dip of the subducting plate affect pat-
            Molnar, 1987; Somoza, 1998; Norabuena et al., 1999).   terns of volcanism. In the central Andes, where the
            Currently, relative motion results in a variable compo-  slab dips steeply, Neogene volcanism is abundant (Plate
            nent of trench-parallel displacement along the margin.   10.1a between pp. 244 and 245). By contrast, above the

            In the central Andes, this component is minor and   flat slab segments of north-central Peru and Chile (30°S

            appears to be accommodated mostly within the sub-  latitude), significant Neogene volcanism is absent.
            ducted slab itself (Siame et al., 2005). In the southern   These volcanic gaps and flat slab segments align with

            Andes, a moderate component of trench-parallel   the location of partially subducted aseismic ridges.
            motion is accommodated by slip along major strike-slip   Gutscher et al. (2000) used relocated earthquake hypo-
            faults (Cembrano et al., 2000, 2002).        centers (Engdahl  et al., 1998) below 70 km depth to
               Focal mechanism solutions from shallow (≤70 km   generate a three-dimensional tomographic image of
            depth) earthquakes show that the South American plate   the subducted Nazca plate beneath the central and
            is currently in compression (Fig. 10.2). Near the Peru–  northern Andes (Plate 10.1b between pp. 244 and 245).
            Chile Trench, some normal faulting occurs in response   The image shows two morphological highs that cor-
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