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Post-perovskite Transition in MgSiO3
Taku Tsuchiya, Jun Tsuchiya, Koichiro Umemoto, and Renata M. Wentzcovitch Dept. of Chemical Engineering and Materials Science , Minnesota Supercomputing Institute UNIVERSITY OF MINNESOTA
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MgSiO3 Perovskite ----- Most abundant constituent in the Earth’s lower mantle ----- Orthorhombic distorted perovskite structure (Pbnm, Z=4) ----- Its stability is important for understanding deep mantle (D” layer)
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UNKNOWN PHASE Pbnm Perovskite
Drastic change in X-ray diffraction pattern around 125 GPa and 2500 K UNKNOWN PHASE Pbnm Perovskite (M. Murakami and K. Hirose, private communication)
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Method --- Density Functional Theory (Hohenberg and Kohn, 1964)
--- Local Density Approximation (Ceperley and Alder, 1985) --- Plane wave basis – pseudopotential (Troullier and Martins, 1991) --- Variable Cell Shape Molecular Dynamics for structural search (Wentzcovitch, 1991)
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Ab initio exploration of post-perovskite phase in MgSiO3
- Reasonable polyhedra type and connectivity under ultra high pressure - SiO4 chain SiO3 layer Perovskite SiO3 Mg MgSiO3
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Crystal structure of post-perovskite
b c a Pt Lattice system: Bace-centered orthorhombic Space group: Cmcm Formula unit [Z]: 4 (4) Lattice parameters [Å] a: (4.286) [120 GPa] b: (4.575) c: (6.286) Volume [120 GPa] [Å3]: (123.3) ( )…perovskite
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A structure has lower energy than Pbnm perovskite under high pressure!
Pt = 98 GPa
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Deformation of perovskite under shear strain ε6
Structural relation between Pv and Post-pv θ Post-perovskite c’ a’ b’ Si-O bonds break Share-edges form Perovskite a b c Deformation of perovskite under shear strain ε6
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Thermodynamics with QHA
--- VDoS and F(T,V) --- Other thermodynamics quantities --- Density Functional Perturbation Theory for calculating phonon frequencies (Gianozzi et al., 1991)
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Thermodynamic properties
( )…Pv Bulk modulus [GPa] [300 K, 0 GPa] B0 222 (248) dB/dP 4.2 (3.9) Ambient volume [cm3/mol] V0 (24.704) Grüneisen parameter γ0 1.6 (1.5) (∂lnγ/∂lnV)T (V/V0) ( (V/V0)) Debye temperature [K] Θ0 1100 (1114)
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High-PT phase diagram 7.5 MPa/K Core-mantle boundary D” layer Hill top
Mantle adiabat error ~5 GPa Core-mantle boundary Hill top Valley bottom ~8 GPa ~250 km 7.5 MPa/K D” layer
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Elasticity of MgSiO3 Post-perovskite
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Post-perovskite : layered structure large compressibility along b axis
Large elastic anisotropy b c Si Large anisotropy as well as large heterogeneity have been observed in D” region Mg a
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Thermoelastic constant tensor CijS(T,P)
kl equilibrium structure re-optimize
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Elastic Constants a c c b b a b a c a
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Aggregate Elastic Moduli
Bppv ≈ Bpv Gppv > Gpv
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Tsuchiya, Tsuchiya, Umemoto,
Single crystal azimuthal anisotropy P-azimuthal: S-azimuthal: Wentzcovitch et al. (1998) Tsuchiya, Tsuchiya, Umemoto, Wentzcovitch, GRL (2004)
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Shear wave splitting in transversely isotropic aggregates
[100] [010] [001] Vertical direction// The degree of polarization anisotropy of shear waves for three crystallographic direction can be determined It is important from the point view of seismology to estimate the anisotropy of a transversely isotropic aggregate of minerals. This figure shows polarization anisotropy as a function of pressure for a transversely isotropic composite of post-perovskite with the a, b, and c axis as a symmetric axis. Post-pv shows very strong polarization anisotropy than pv. Lattice preferred orientation of post-PV polycrystals can produce seismically detectable anisotropy in the bottom of lower mantle. Vsh Vsv Horizontal plane
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Seismic velocities <
Longitudinal Shear Bulk Post-pv transition should produce larger anomaly in VS than in VP
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Summary -10% < AST < 15%
Post-pv phase has almost the same B as pv but larger G Across the transition at 125 GPa (2750 K) Δρ ~ 1.5% ΔVS ~ 1.5% > ΔVP ~ 1% ΔVΦ ~ -0.7% Post-pv has larger dV/dT’s Lateral ΔT → ΔVppv> ΔVpv Post-pv is very anisotropic at D” conditions Perfect transversely isotropic aggregates -10% < AST < 15%
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Acknowledgements Thanks to Murakami and Hirose for early communication of their X-ray diffraction NSF COMPRES, NSF/EAR
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