A geodynamic model of plumes from the margins of Large Low Shear Velocity Provinces

[1] We present geodynamic models featuring mantle plumes that are almost exclusively created at the margins of large thermo-chemical piles in the lowermost mantle. The models are based on subduction locations and fluxes inferred from global plate reconstructions and ocean floor paleo-ages. Sinking subducted slabs not only push a heavy chemical layer ahead, such that dome-shaped structures form, but also push the thermal boundary layer (TBL) toward the chemical domes. At the steep edges it is forced upwards and begins to rise — in the lower part of the mantle as sheets, which then split into individual plumes higher in the mantle. The models explain why Large Igneous Provinces – commonly assumed to be caused by plumes forming in the TBL above the core-mantle boundary (CMB)– and kimberlites during the last few hundred Myr erupted mostly above the margins of the African and Pacific Large Low Shear Velocity Provinces (LLSVPs) of the lowermost mantle, which are probably chemically distinct from and heavier than the overlying mantle. Our models support that mantle plumes are more intimately linked to plate tectonics than commonly believed. Not only can plumes cause continental break-up, but conversely subducted plates may trigger plumes at the margins of LLSVPs near the CMB.

[1]  S. Zhong,et al.  Core–mantle boundary topography as a possible constraint on lower mantle chemistry and dynamics , 2010 .

[2]  H. Nataf Mantle convection, plates, and hotspots , 1991 .

[3]  Sri Widiyantoro,et al.  Global seismic tomography: A snapshot of convection in the Earth: GSA Today , 1997 .

[4]  H. Bunge,et al.  Tomographic images of a mantle circulation model , 2001 .

[5]  M. Gurnis THE EFFECTS OF CHEMICAL DENSITY DIFFERENCES ON CONVECTIVE MIXING IN THE EARTH'S MANTLE , 1986 .

[6]  M. Monnereau,et al.  Spherical shell models of mantle convection with tectonic plates , 2001 .

[7]  P. Tackley Three‐Dimensional Simulations of Mantle Convection with a Thermo‐Chemical Basal Boundary Layer: D″? , 2013 .

[8]  G. Davies,et al.  Ocean bathymetry and mantle convection: 1. Large‐scale flow and hotspots , 1988 .

[9]  D. Antonangeli,et al.  Effect of composition, structure, and spin state on the thermal conductivity of the Earth's lower mantle , 2010 .

[10]  M. Manga,et al.  The influence of a chemical boundary layer on the fixity, spacing and lifetime of mantle plumes , 2002, Nature.

[11]  B. Romanowicz,et al.  Mantle Anchor Structure: An argument for bottom up tectonics , 2010 .

[12]  Edward J. Garnero,et al.  Geographic correlation between hot spots and deep mantle lateral shear-wave velocity gradients , 2004 .

[13]  P. Tackley Living dead slabs in 3-D: The dynamics of compositionally-stratified slabs entering a "slab graveyard" above the core-mantle boundary , 2011 .

[14]  B. Steinberger,et al.  Large igneous provinces generated from the margins of the large low-velocity provinces in the deep mantle , 2006 .

[15]  McSween Hy,et al.  Evidence for Life in a Martian Meteorite , 1997 .

[16]  B. Hager,et al.  Understanding the effects of mantle compressibility on geoid kernels , 1996 .

[17]  W. Press,et al.  Numerical Recipes: The Art of Scientific Computing , 1987 .

[18]  P. Olson,et al.  Experiments on the interaction of thermal convection and compositional layering at the base of the mantle , 1991 .

[19]  B. Steinberger Plumes in a convecting mantle: Models and observations for individual hotspots , 2000 .

[20]  R. Müller,et al.  Global plate motion frames: Toward a unified model , 2008 .

[21]  F. D. Stacey,et al.  The dynamical and thermal structure of deep mantle plumes , 1983 .

[22]  L. Wen,et al.  Mapping the geometry and geographic distribution of a very low velocity province at the base of the Earth's mantle , 2004 .

[23]  P. Tackley,et al.  Deep mantle heat flow and thermal evolution of the Earth's core in thermochemical multiphase models of mantle convection , 2005 .

[24]  N. Koker Thermal conductivity of MgO periclase at high pressure: Implications for the D″ region , 2010 .

[25]  J. Tromp,et al.  Constraining large-scale mantle heterogeneity using mantle and inner-core sensitive normal modes , 2004 .

[26]  W. J. Morgan,et al.  Convection Plumes in the Lower Mantle , 1971, Nature.

[27]  Anne M. Hofmeister,et al.  Inference of high thermal transport in the lower mantle from laser-flash experiments and the damped harmonic oscillator model , 2008 .

[28]  M. Gurnis,et al.  Slabs in the lower mantle and their modulation of plume formation , 2002 .

[29]  B. Steinberger,et al.  Conduit diameter and buoyant rising speed of mantle plumes: Implications for the motion of hot spots and shape of plume conduits , 2006 .

[30]  Lapo Boschi,et al.  A comparison of tomographic and geodynamic mantle models , 2002 .

[31]  Thorne Lay,et al.  Core–mantle boundary heat flow , 2008 .

[32]  Jeroen Ritsema,et al.  Synthetic tomography of plume clusters and thermochemical piles , 2009 .

[33]  Joseph S. Resovsky,et al.  Probabilistic Tomography Maps Chemical Heterogeneities Throughout the Lower Mantle , 2004, Science.

[34]  T. Lay,et al.  Partial melting in a thermo-chemical boundary layer at the base of the mantle , 2004 .

[35]  T. Torsvik,et al.  Toward an explanation for the present and past locations of the poles , 2010 .

[36]  N. Zhang,et al.  Supercontinent formation from stochastic collision and mantle convection models , 2009 .

[37]  W. J. Morgan,et al.  Deep Mantle Convection Plumes and Plate Motions , 1972 .

[38]  L. Stixrude,et al.  Thermal conductivity of periclase (MgO) from first principles. , 2010, Physical review letters.

[39]  B. Steinberger,et al.  Absolute plate motions and true polar wander in the absence of hotspot tracks , 2008, Nature.

[40]  Mark A. Richards,et al.  Plume capture by divergent plate motions: implications for the distribution of hotspots, geochemistry of mid-ocean ridge basalts, and estimates of the heat flux at the core–mantle boundary , 2003 .

[41]  Mark Turner,et al.  Plate tectonic reconstructions with continuously closing plates , 2012, Comput. Geosci..

[42]  John Hernlund,et al.  On the statistical distribution of seismic velocities in Earth's deep mantle , 2008 .

[43]  E. Garnero,et al.  Structure and Dynamics of Earth's Lower Mantle , 2008, Science.

[44]  É. Stutzmann,et al.  Convective patterns under the Indo-Atlantic « box » , 2005 .

[45]  B. Hager,et al.  Kinematic models of large‐scale flow in the Earth's mantle , 1979 .

[46]  Bradford H. Hager,et al.  A simple global model of plate dynamics and mantle convection , 1981 .

[47]  Maisha Amaru,et al.  Towards absolute plate motions constrained by lower-mantle slab remnants , 2010 .

[48]  Walter H. F. Smith,et al.  New, improved version of generic mapping tools released , 1998 .

[49]  Julian P. Lowman,et al.  Mantle Convection in the Earth and Planets , 2002 .

[50]  M. Richards,et al.  Modulation of mantle plumes and heat flow at the core mantle boundary by plate-scale flow: results from laboratory experiments , 2004 .

[51]  Adam M. Dziewonski,et al.  Mapping the lower mantle: Determination of lateral heterogeneity in P velocity up to degree and order 6 , 1984 .

[52]  Eh Tan,et al.  GeoFramework: Coupling multiple models of mantle convection within a computational framework , 2006 .

[53]  B. Steinberger,et al.  Advection of plumes in mantle flow: implications for hotspot motion, mantle viscosity and plume distribution , 1998 .

[54]  B. Hager,et al.  Onset of mantle plumes in the presence of preexisting convection , 1988 .

[55]  J. Wilson A possible origin of the Hawaiian Islands , 1963 .

[56]  Shijie Zhong,et al.  Thermochemical structures beneath Africa and the Pacific Ocean , 2005, Nature.

[57]  Eh Tan,et al.  Metastable superplumes and mantle compressibility , 2005 .

[58]  A. Davaille,et al.  On the transient nature of mantle plumes , 2005 .

[59]  P. Beck,et al.  Thermal conductivity of lower-mantle minerals , 2009 .

[60]  M. Gurnis,et al.  On the location of plumes and lateral movement of thermochemical structures with high bulk modulus in the 3‐D compressible mantle , 2011 .

[61]  T. Lay,et al.  Implications of lower-mantle structural heterogeneity for the existence and nature of whole-mantle plumes , 2007 .

[62]  B. Steinberger,et al.  Models of large‐scale viscous flow in the Earth's mantle with constraints from mineral physics and surface observations , 2006 .

[63]  W. Leng,et al.  A model for the evolution of the Earth's mantle structure since the Early Paleozoic , 2010 .

[64]  Kevin Burke,et al.  Plume Generation Zones at the margins of Large Low Shear Velocity Provinces on the core–mantle boundary , 2008 .

[65]  J. Korenaga Firm mantle plumes and the nature of the core–mantle boundary region , 2005 .

[66]  L. Boschi,et al.  Mantle plumes: Dynamic models and seismic images , 2007 .

[67]  D. Helmberger,et al.  Sharp Sides to the African Superplume , 2002, Science.

[68]  A. Jellinek,et al.  Transient mantle convection on Venus: The paradoxical coexistence of highlands and coronae in the BAT region , 2007 .

[69]  M. Richards,et al.  Flood Basalts and Hot-Spot Tracks: Plume Heads and Tails , 1989, Science.

[70]  Norman H. Sleep,et al.  Hotspots and Mantle Plumes' Some Phenomenology , 1990 .

[71]  D. Anderson,et al.  Hotspots, basalts, and the evolution of the mantle. , 1981, Science.

[72]  D. L. Anderson,et al.  Preliminary reference earth model , 1981 .

[73]  U. Christensen,et al.  The excess temperature of plumes rising from the core‐mantle boundary , 1996 .

[74]  B. Steinberger,et al.  Diamonds sampled by plumes from the core–mantle boundary , 2010, Nature.

[75]  É. Stutzmann,et al.  Convective patterns under the Indo-Atlantic T box r , 2005 .

[76]  Gabi Laske,et al.  The Relative Behavior of Shear Velocity, Bulk Sound Speed, and Compressional Velocity in the Mantle: Implications for Chemical and Thermal Structure , 2013 .