Spawning superplumes from the midmantle: The impact of spin transitions in the mantle

The formation of large scale upwellings with lateral extents of several hundreds of kilometers, reaching up to ∼10000 km or more, still remains a hotly debated topic. Some seismic imaging studies based on high resolution data suggest that the main superplumes underneath Africa and South-central Pacific are clusters, composed of several individual plumes rather than being a single large mantle upwelling. The iron spin transition in the lower mantle minerals may present a new idea on the origin and the formation of such superplumes, notably sourcing such features in the mid-mantle. Stagnation of both cold sinking slabs and hot rising plumes can be caused by density and viscosity variation due to the spin transition in iron in ferropericlase (Fp) and a possible spin-dependent bulk modulus hardening in bridgmanite silicate perovskite (Pv). This process produces intermittent downward spin transition-induced mid-mantle avalanches (SIMMA) of the cold sinking flow as well as upward spin transition-induced mid-mantle superplume avalanches (SIMMSA) of the rising hot plumes, triggered at the spin transition-induced thermal boundary layer at around 1600 km depth. Our high resolution axi-symmetric models reveal that the hot upwellings, trapped below ∼1600 km depth, can suddenly penetrate into the upper levels in the mantle and spread laterally for hundreds of kilometres. Owing to the upward penetration of the mid-mantle rooted superplumes, as broad as ∼1500 km across, a large amount of heat can be delivered to the upper mantle and base of the lithosphere with implications for large volcanic episodes. This article is protected by copyright. All rights reserved.

[1]  Robert W. Clayton,et al.  Lower mantle heterogeneity, dynamic topography and the geoid , 1985, Nature.

[2]  J. Ritsema,et al.  African hot spot volcanism: small-scale convection in the upper mantle beneath cratons. , 2000, Science.

[3]  D. Yuen,et al.  Superplumes: Beyond Plate Tectonics , 2007 .

[4]  Y. Ohishi,et al.  Post-Perovskite Phase Transition in MgSiO3 , 2004, Science.

[5]  Masaki Yoshida Temporal evolution of the stress state in a supercontinent during mantle reorganization , 2010 .

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

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

[8]  T. Ruedas,et al.  Pressure‐ and temperature‐dependent thermal expansivity and the effect on mantle convection and surface observables , 2002 .

[9]  R. Pysklywec,et al.  Anomalous bathymetry, 3D edge driven convection, and dynamic topography at the western Atlantic passive margin , 2011 .

[10]  Barbara Romanowicz,et al.  Broad plumes rooted at the base of the Earth's mantle beneath major hotspots , 2015, Nature.

[11]  D. Yuen,et al.  Viscosity undulations in the lower mantle: The dynamical role of iron spin transition , 2015 .

[12]  H. Watson,et al.  Predominant Intermediate-Spin Ferrous Iron in Lowermost Mantle Post-Perovskite and Perovskite , 2008 .

[13]  Renata M. Wentzcovitch,et al.  The high‐pressure electronic spin transition in iron: Potential impacts upon mantle mixing , 2011 .

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

[15]  B. Windley,et al.  History of the Pacific Superplume: Implications for Pacific Paleogeography Since the Late Proterozoic , 2007 .

[16]  Kenneth G. Dueker,et al.  Beneath Yellowstone: Evaluating Plume and Nonplume Models Using Teleseismic Images of the Upper Mantle , 2000 .

[17]  R. Jeanloz,et al.  Iron spin transition in Earth's mantle. , 2005, Proceedings of the National Academy of Sciences of the United States of America.

[18]  Guillaume Fiquet,et al.  Electronic Transitions in Perovskite: Possible Nonconvecting Layers in the Lower Mantle , 2004, Science.

[19]  Renata M. Wentzcovitch,et al.  Spin crossover in ferropericlase and velocity heterogeneities in the lower mantle , 2014, Proceedings of the National Academy of Sciences.

[20]  R. Larson Geological consequences of superplumes , 1991 .

[21]  Guust Nolet,et al.  A catalogue of deep mantle plumes: New results from finite‐frequency tomography , 2006 .

[22]  S. Karato,et al.  Shear deformation of bridgmanite and magnesiowüstite aggregates at lower mantle conditions , 2016, Science.

[23]  D. Yuen,et al.  Anomalous compressibility of ferropericlase throughout the iron spin cross-over , 2009, Proceedings of the National Academy of Sciences.

[24]  W. J. Morgan,et al.  Imaging the mantle beneath Iceland using integrated seismological techniques , 2002 .

[25]  Enhanced convection and fast plumes in the lower mantle induced by the spin transition in ferropericlase , 2009 .

[26]  R. Pysklywec,et al.  Anomalous topography in the western Atlantic caused by edge‐driven convection , 2004 .

[27]  W. Peltier,et al.  Layered convection and the impacts of the perovskite-postperovskite phase transition on mantle dynamics under isochemical conditions , 2010 .

[28]  Sang-Heon Shim,et al.  Effects of the Fe3 + spin transition on the properties of aluminous perovskite—New insights for lower-mantle seismic heterogeneities , 2011 .

[29]  L. Kellogg,et al.  Effect of mantle plumes on the growth of D” by reaction between the core and mantle , 1993 .

[30]  Y. Meng,et al.  Spin transition and equations of state of (Mg, Fe)O solid solutions , 2007 .

[31]  B. Romanowicz,et al.  Superplumes from the Core-Mantle Boundary to the Lithosphere: Implications for Heat Flux , 2002, Science.

[32]  A. Hofmeister,et al.  Mantle values of thermal conductivity and the geotherm from phonon lifetimes , 1999, Science.

[33]  Satoshi Kaneshima,et al.  Seismic scatterers in the mid-lower mantle , 2016 .

[34]  G. Barruol,et al.  South Pacific hotspot swells dynamically supported by mantle flows , 2010 .

[35]  H. Shiobara,et al.  South Pacific mantle plumes imaged by seismic observation on islands and seafloor , 2009 .

[36]  A. Tsuchiyama,et al.  Low Core-Mantle Boundary Temperature Inferred from the Solidus of Pyrolite , 2014, Science.

[37]  Stefano de Gironcoli,et al.  Anomalous thermodynamic properties in ferropericlase throughout its spin crossover transition , 2009 .

[38]  W. R. Peltier,et al.  Deepest mantle viscosity: Constraints from Earth rotation anomalies , 2010 .

[39]  J. Badro,et al.  Spin state transition and partitioning of iron: Effects on mantle dynamics , 2015 .

[40]  Guillaume Fiquet,et al.  Iron Partitioning in Earth's Mantle: Toward a Deep Lower Mantle Discontinuity , 2003, Science.

[41]  Shijie Zhong,et al.  Thermochemical structures within a spherical mantle: Superplumes or piles? , 2004 .

[42]  J. Dohm,et al.  THARSIS SUPERPLUME AND THE GEOLOGICAL EVOLUTION OF EARLY MARS , 2007 .

[43]  E. Engdahl,et al.  Finite-Frequency Tomography Reveals a Variety of Plumes in the Mantle , 2004, Science.

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

[45]  D. L. Anderson Hawaii, Boundary Layers and Ambient Mantle—Geophysical Constraints , 2011 .

[46]  D. L. Anderson Scoring hotspots: The plume and plate paradigms , 2005 .

[47]  R. Ernst,et al.  Plumes and Plume Clusters on Earth and Venus: Evidence from Large Igneous Provinces (LIPs) , 2007 .

[48]  David A. Yuen,et al.  The importance of radiative heat transfer on superplumes in the lower mantle with the new post-perovskite phase change , 2005 .

[49]  John H. Woodhouse,et al.  Mapping the upper mantle: Three‐dimensional modeling of earth structure by inversion of seismic waveforms , 1984 .

[50]  T. Lay,et al.  Mineralogy of the Deep Mantle – The Post-Perovskite Phase and its Geophysical Significance , 2015 .

[51]  Sang-Heon Shim,et al.  Spin state of ferric iron in MgSiO3 perovskite and its effect on elastic properties , 2010 .

[52]  A. Hofmeister Thermal Conductivity of the Earth's Deepest Mantle , 2007 .

[53]  Jean Besse,et al.  Three distinct types of hotspots in the Earth's mantle , 2002 .

[54]  Stefano de Gironcoli,et al.  Spin transition in magnesiowüstite in earth's lower mantle. , 2006, Physical review letters.

[55]  David A. Yuen,et al.  Dynamics of Superplumes in the Lower Mantle , 2007 .

[56]  R. Larson Latest pulse of Earth: Evidence for a mid-Cretaceous superplume , 1991 .

[57]  G. Schubert,et al.  Superplumes or plume clusters , 2004 .

[58]  W. R. Peltier,et al.  The impacts of mantle phase transitions and the iron spin crossover in ferropericlase on convective mixing—is the evidence for compositional convection definitive? New results from a Yin‐Yang overset grid‐based control volume model , 2015 .

[59]  Robert D. van der Hilst,et al.  Searching for seismic scattering off mantle interfaces between 800 km and 2000 km depth , 2003 .

[60]  J. Wilson,et al.  A New Class of Faults and their Bearing on Continental Drift , 1965, Nature.

[61]  P. Tackley Strong heterogeneity caused by deep mantle layering , 2002 .