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THE MECHANISM OF PLATE TECTONICS  395



            to rise from the thermal boundary layer at the core–  12.8.4 The D″ layer
            mantle boundary (Plate 12.2 between pp. 244 and 245)
            (Section 12.8.4).
               Just as upwellings in the mantle produce regional   It has long been recognized that the greatest contrasts
            uplift of the Earth’s surface, downwellings produce   in physical properties and chemical composition within
            regional subsidence (Gurnis, 2001). The most notable   the Earth occur at the core–mantle boundary and that
            example of depressed crust at the present day is the   this is almost certainly the location of a thermo-chemi-
            Indonesian region. This is situated above anomalously   cal boundary layer (Section 2.8.6). Initially, seismolo-
            high seismic velocities in the transition zone and upper   gists were unable to detect any layering in the lower
            part of the lower mantle (Plate 12.2b between pp. 244   mantle and referred to it as Layer D (Bullen, 1949).

            and 245) that probably reflect a confluence of downgo-  Subsequently it was realized that a layer at the base of

            ing lithospheric slabs. Seismic tomography can only   the mantle, perhaps 2–300 km thick, has distinctive, if
            map regions of low and high velocity, and hence pos-  variable, characteristics; typically lower seismic veloci-
            sible upwellings and downwellings in the mantle, at   ties or a lower velocity gradient than in the lower
            the present day. However, evidence from the geologic   mantle above. Hence the lower mantle is now divided
            record for regional scale elevation and subsidence of   into two seismologic layers D′ and D″. With further
            the Earth’s crust may indicate that a particular area   refinements in seismologic techniques, studies of


            has been underlain by a major mantle upwelling or   seismic waves reflected, refracted and diffracted at the
            deep subducting slabs in the past. Originally it was   core–mantle boundary have revealed remarkable details
            assumed that changes in sea level, causing major marine   of the complexity and lateral variability of layer D″.
            transgressions and regressions on continental crust,   The geographic distribution of earthquakes and seis-
            were synchronous worldwide, away from areas of   mologic observatories is such that not all parts of the
            active tectonism. However, as more data accumulated   layer can be studied in the same degree of detail. Clearly
            it became clear that this was not so, although an   for such a remote layer, that is now thought to have
            obvious explanation was lacking. It is now apparent   vertical and horizontal variability analogous to that of
            that elevation and subsidence of the lithosphere associ-  the lithosphere, this poses quite a challenge for future
            ated with convection in the mantle, could provide an   seismologic studies.
            explanation for what were previously some very enig-  Figure 12.11 illustrates the picture that is emerging
            matic observations.                          of the nature of layer D″ for three very different regions
               Denver, Colorado in the central USA has an eleva-  for which detailed studies have been possible: beneath
            tion of 1.6 km but is underlain by Cretaceous sediments   central America, Hawaii, and southern Africa. The
            typical of shallow water deposition. At that time the   upper boundary of the layer is characterized by a veloc-

            Farallon plate, the eastern flank of the East Pacifi c Rise   ity discontinity. Below this there may be an increase or

            in the northeast Pacific, was being subducted beneath   decrease in the seismic velocities, particularly the shear
            western and central North America and is thought to   wave velocity, or a decrease in the velocity gradient with
            have caused depression of the crust above it. With the   depth. A velocity increase is most marked beneath
            progressive elimination of the East Pacific Rise in the   regions where there are subducting slabs such as Central

            northeast Pacific throughout the late Cenozoic, the Far-  America (Fig. 12.11a). In a 5- to 50-km-thick layer imme-

            allon plate has become detached and continues to sink   diately above the core–mantle boundary there is often
            eastwards, allowing the buoyancy of the crust of the   a zone of ultra-low seismic velocities, with decreases in
            western and central USA to reassert itself, thereby   the shear wave velocity of 10–50%. This implies partial
            causing the uplift of the Colorado region. Van der Hilst   melting with more than 15% melt (Thybo et al., 2003).
            et al. (1997), using seismic tomography, imaged the   These ultra-low velocity zones (ULVZ) are most exten-
            sinking Farallon plate 1600 km beneath the eastern   sively developed beneath major hotspots such as Hawaii
            USA. Similar anomalous vertical movements of parts of   (Fig. 12.11b) and beneath the superswells, and inferred

            Australia since the early Cretaceous are thought to be   upwellings, of the central Pacific and southern Africa

            due to the influence of downwellings created by sub-  (Fig. 12.11c). Unlike the variations in seismic velocity in
            duction zones, initially to the east of Australia, and   the main part of the lower mantle, that are thought to
            more recently to the north (Gurnis et al., 1998).  be largely due to temperature differences, the marked
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