The structure of the core‐mantle boundary from diffracted waves

Diffracted P and S waves (Pd, Sd) traveling around the core-mantle boundary (CMB) of the Earth give us information about the velocity structure and therefore the thermochemistry of D″, the base of the Earth's mantle. By examining Pd and Sdarrivals we determined the apparent ray parameter for different regions at the base of the mantle. By comparing the data slownesses to those found from reflectivity synthetic seismograms we were able to quantify D″ average velocities. Using these averaged velocities with a thermochemical modeling of lower mantle minerals using a Birch-Mumaghan equation of state, we have been able to make chemical and physical inferences as to the causes of lateral variations at the CMB. Examinations found significant lateral heterogeneity at the base of the mantle, amounting to ≈ 4% for both P and S velocities. These velocities did not always vary in parallel, and the Poisson ratio varied regionally by almost 6%. The most unusual region of the CMB found was under Indonesia, where velocities 3% slower than the preliminary reference Earth models were found adjacent to a region of faster than average velocities. These regions currently correspond to areas of core up welling and down welling (respectively) found by Voorhies (1986), which if mostly held in place by core-mantle coupling might cause a flux of heat and iron into the mantle, making the anomaly both thermally and chemically derived. At the CMB under the northern Pacific rim the fastest shear velocities were found, but the same region yielded slower than average P velocities. While the presence of fast shear velocities here would support the idea that we are seeing the cold dregs of mantle convection, perhaps continuing down from the North Pacific subduction zones, the presence of slow P velocities suggests additional complications. Our thermochemical modeling suggests that the D″ Poisson ratio is very sensitive to variations in the silicate/oxide ratio and that a decrease in the amount of perovskite relative to magnesiowustite may play an important role in this region.

[1]  K. Bullen Compressibility-Pressure Hypothesis and the Earth's Interior , 1949 .

[2]  D. Jault,et al.  Core-mantle boundary shape: constraints inferred from the pressure torque acting between the core and the mantle , 1990 .

[3]  W. H. Ramsey On the Nature of the Earth's Core , 1949 .

[4]  F. Birch Elasticity and Constitution of the Earth's Interior , 1952 .

[5]  T. Jordan,et al.  Mantle layering from ScS reverberations: 4. The lower mantle and core-mantle boundary , 1991 .

[6]  C. Young,et al.  The Core-Mantle Boundary , 1987 .

[7]  I. Sacks Diffracted P‐wave studies of the Earth's core: 2. Lower mantle velocity, core size, lower mantle structure , 1967 .

[8]  D. Yuen,et al.  Dynamical effects on the core‐mantle boundary from depth‐dependent thermodynamical properties of the lower mantle , 1988 .

[9]  R. Phinney,et al.  A study of the core-mantle boundary using P waves diffracted by the Earth's core , 1966 .

[10]  J. Bloxham Simple models of fluid flow at the core surface derived from geomagnetic field models , 1989 .

[11]  Hiroo Kanamori,et al.  Mode of the strain release along the Gibbs fracture zone, Mid-Atlantic ridge , 1976 .

[12]  Jeremy Bloxham,et al.  Fluid flow near the surface of Earth's outer core , 1991 .

[13]  R. Carlson,et al.  The large-scale structure of convection in the Earth's mantle , 1990, Nature.

[14]  D. Jault,et al.  The topographic torque associated with a tangentially geostrophic motion at the core surface and inferences on the flow inside the core , 1989 .

[15]  Don L. Anderson,et al.  Travel times and station corrections for P waves at teleseismic distances , 1983 .

[16]  D. J. Doornbos,et al.  Attenuation of P and S waves diffracted around the core , 1979 .

[17]  V. Cormier Slab diffraction of S waves , 1989 .

[18]  N. Srivastava,et al.  Fault plane solutions as related to known geological faults in and near India , 1975 .

[19]  D. Giardini Systematic analysis of deep seismicity: 200 centroid-moment tensor solutions for earthquakes between 1977 and 1980 , 1984 .

[20]  O. Anderson,et al.  Measured elastic moduli of single-crystal MgO up to 1800 K , 1989 .

[21]  T. Tanimoto The three-dimensional shear wave structure in the mantle by overtone waveform inversion - I. Radial seismogram inversion , 1987 .

[22]  A. Mula Amplitudes of diffracted long‐period P and S waves and the velocities and Q structure at the base of the mantle , 1981 .

[23]  Raymond Jeanloz,et al.  Phase transitions and mantle discontinuities , 1983 .

[24]  G. Müller,et al.  Ray parameters of diffracted long period P and S waves and the velocities at the base of the mantle , 1980 .

[25]  A. Ringwood Composition and petrology of the earth's mantle , 1975 .

[26]  G. Schubert,et al.  Influence of heating mode on three-dimensional mantle convection , 1989 .

[27]  A. L. Hales,et al.  Shear velocities in the lower mantle and the radius of the core , 1970 .

[28]  C. Chapman,et al.  Diffracted Seismic Signals and Their Numerical Solution , 1972 .

[29]  G. L. Choy Theoretical seismograms of core phases calculated by frequency‐dependent full wave theory, and their interpretation , 1977 .

[30]  A. Agnon,et al.  High pressure shear moduli—A many body model for oxides , 1988 .

[31]  N. Sleep Gradual entrainment of a chemical layer at the base of the mantle by overlying convection , 1988 .

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

[33]  D. Weidner,et al.  Elasticity of MgSiO3 in the Perovskite Structure , 1989, Science.

[34]  Thomas J. Ahrens,et al.  The equation of state of Mg0.6Fe0.4O to 200 GPa , 1982 .

[35]  R. Jeanloz,et al.  Simulating the core‐mantle boundary: An experimental study of high‐pressure reactions between silicates and liquid iron , 1989 .

[36]  T. Lay,et al.  Investigation of laterally heterogeneous shear velocity structure in D″ beneath Eurasia , 1992 .

[37]  R. Jeanloz,et al.  Synthesis and Equation of State of (Mg,Fe) SiO3 Perovskite to Over 100 Gigapascals , 1987, Science.

[38]  P. Molnar,et al.  Focal mechanisms along inclined earthquake zones, in the Indonesia-Philippine region , 1970 .

[39]  E. Okal,et al.  Shear-wave velocity at the base of the mantle from profiles of diffracted SH waves , 1979, Bulletin of the Seismological Society of America.

[40]  P. Silver,et al.  Constraints on lower mantle composition and temperature from density and bulk sound velocity profiles , 1990 .

[41]  P. Molnar,et al.  Focal mechanisms and plate tectonics of the southwest Pacific , 1972 .

[42]  A. Espinosa P in the shadow zone of the earth's core—Part I , 1967 .

[43]  M. Gurnis,et al.  Interaction of mantle dregs with convection: Lateral heterogeneity at the core‐mantle boundary , 1986 .

[44]  H. Mao,et al.  Effect of pressure, temperature, and composition on lattice parameters and density of (Fe,Mg)SiO3‐perovskites to 30 GPa , 1991 .

[45]  R. Jeanloz,et al.  Melting curve of (Mg,Fe)SiO3 perovskite to 96 GPa: Evidence for a structural transition in lower mantle melts , 1989 .

[46]  Albrecht W. Hofmann,et al.  Mantle plumes from ancient oceanic crust , 1982 .

[47]  R. Jeanloz,et al.  The high‐pressure phase diagram of Fe0.94O: A possible constituent of the Earth's core , 1991 .

[48]  P. Molnar,et al.  Distribution of stresses in the descending lithosphere from a global survey of focal‐mechanism solutions of mantle earthquakes , 1971 .

[49]  Jeremy Bloxham,et al.  Simultaneous stochastic inversion for geomagnetic main field and secular variation: 2. 1820–1980 , 1989 .

[50]  U. Chandra On the focal mechanism of the Peru-Bolivia border earthquake of August 15, 1963 , 1970, Bulletin of the Seismological Society of America.

[51]  Yosihiko Ogata,et al.  Whole mantle P-wave travel time tomography , 1990 .

[52]  T. Fitch Earthquake mechanisms and island arc tectonics in the Indonesian-Philippine region , 1970 .

[53]  Andrea Morelli,et al.  Topography of the core–mantle boundary and lateral homogeneity of the liquid core , 1987, Nature.

[54]  E. Ito,et al.  Stability Relations of Silicate Spinels, Ilmenites, and Perovskites , 1982 .

[55]  R. Gordon,et al.  Current plate velocities relative to the hotspots incorporating the NUVEL-1 global plate motion model , 1990 .

[56]  E. Okal,et al.  Regional analysis of D″ velocities from the ray parameters of diffracted P profiles , 1989 .

[57]  J. Mondt SH waves: Theory and observations for epicentral distances greater than 90 degrees , 1977 .

[58]  B. Romanowicz,et al.  Observational evidence for diffracted SV in the shadow of the Earth's core , 1989 .

[59]  G. Wolf,et al.  Thermodynamically consistent decompression: Implications for lower mantle composition , 1990 .

[60]  T. Lay Structure of the core‐mantle transition zone , 1989 .

[61]  T. Lay,et al.  A lower mantle S-wave triplication and the shear velocity structure of D" , 1983 .

[62]  C. Voorhies Steady flows at the top of Earth's core derived from geomagnetic field models , 1986 .

[63]  K. Jacob,et al.  Investigation of the Dynamical Process in Earthquake Foci by Analyzing the Pulse Shape of Body Waves. , 1968 .

[64]  D. J. Doornbos,et al.  P and S waves diffracted around the core and the velocity structure at the base of the mantle , 1979 .

[65]  L. Sykes,et al.  Seismicity and tectonics of the western Pacific: Izu-Mariana-Caroline and Ryukyu-Taiwan regions , 1969 .

[66]  D. Yuen,et al.  Dynamical influences from thermal‐chemical instabilities at the core‐mantle boundary , 1989 .

[67]  M. Richards,et al.  Hotspots, mantle plumes, flood basalts, and true polar wander , 1991 .

[68]  B. Bolt,et al.  Diffracted ScS and the Shear Velocity at the Core Boundary , 1970 .

[69]  D. Gubbins,et al.  Thermal core– mantle interactions , 1987, Nature.

[70]  D. Stevenson On the role of surface tension in the migration of melts and fluids , 1986 .

[71]  R. Jeanloz,et al.  Synthesis and Equation of State of (Mg,Fe)SiO3 Perovskite to Over 100 Gigapascals. , 1987 .

[72]  D. Jurdy,et al.  Subducted lithosphere, hotspots, and the geoid , 1980 .

[73]  B. Bolt,et al.  S velocities in D" from diffracted SH-waves at the core boundary , 1984 .

[74]  C. Bina,et al.  CALCULATION OF ELASTIC PROPERTIES FROM THERMODYNAMIC EQUATION OF STATE PRINCIPLES , 1992 .

[75]  B. Bolt PdP and PKiKP Waves and Diffracted PcP Waves , 1970 .

[76]  J. Cleary The S velocity at the core-mantle boundary, from observations of diffracted S , 1969 .