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Physics of the Earth and Planetary Interiors 153 (2005) 1-2
Editorial Studies of the Earth's Deep Interior - Eighth Symposium The Eighth Symposium on the Study of the Earth's Deep Interior (SEDI) was held at Garmisch-Partenkirchen, Germany, in the Bavarian Alps, from 4 to 9 July 2004. The meeting attracted about 150 participants to a varied program that expanded the range of topics from previous meetings, with somewhat more emphasis on the mantle, in addition to mantlecore interaction, and core studies. On this occasion attention was also turned to the deep interior of other planets as well as the Earth. FIGURE CAPTION Fig. 1. Schematic cross-section of the Earth’s interior displaying several recent ideas, many of which were highlighted at the Eighth SEDI Symposium. The mantle is shown with large scale convective motions (large arrows), primarily driven by subduction of dense, cold lithosphere (darker outer layer and dark slabs). Whole mantle plumes are most likely to form near or above the hottest deep regions, possibly guided by topographical features in the DTCP. The dominant upper mantle phase boundaries near 410 and 660 km depth are deflected by thermal and/or chemical heterogeneity (e.g., slabs and plumes). Other boundaries have also been detected (e.g., the 220 and 520 km discontinuities, dashed). Lower mantle dense thermochemical piles (DTCP) may be reservoirs of incompatible elements and preferentially locate beneath large scale return flow in the overlying mantle. Seismological studies characterize significant shear velocity reductions in the DTCP, which may be the hottest zones in the lowermost mantle, and thus related to partially molten material that comprises ultra-low velocity zones (ULVZ) right at the coremantle boundary (CMB). The dominant lower mantle mineral structure, magnesium-silicate perovskite, is predicted to transform to a denser phase, post-perovskite (ppv) in the lowermost few hundred km of the mantle (D"); if slabs have a dominantly MgSi perovskite chemistry, then subducted material may independently transform to ppv (white dashed lines near D" in slabs), though this depends on the poorly constrained Capeyron slope of this phase boundary. Thus, heterogeneity in the mantle appears multi-scaled, from the km level (or smaller) to 1000s of km. Convective motions throughout the planet are likely similarly multi-scaled. Abundant evidence now exists for seismic wave speed anisotropy (stippled or grainy areas) near key boundary layers: in the 100s of km below the surface, in the lowermost few hundred km of the mantle (the D" region), and in the inner core. The onset of anisotropy in the inner core (dashed line) may be displaced some 100200 km below the inner core boundary (ICB), and has been characterized as having a fast propagation direction aligned similar to, but slightly offset from Earth’s rotation axis. The innermost inner core may have its own unique subdivision (slightly darker shading). Taylor roll convection is depicted in the outer core (spiral arrows), and lower mantle heterogeneity may affect heat flow from and hence convective flow within the core. Edward J. Garnero Brian Kennett David E. Loper Corresponding author. |
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