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Thermoelasticity of Fe$^{3+}$- and Al-bearing bridgmanite

Published 29 Mar 2016 in cond-mat.mtrl-sci and cond-mat.str-el | (1603.08899v1)

Abstract: We report \textit{ab initio} (LDA + U${sc}$) calculations of thermoelastic properties of ferric iron (Fe${3+}$)- and aluminum (Al)-bearing bridgmanite (MgSiO$_3$ perovskite), the main Earth forming phase, at relevant pressure and temperature conditions and compositions. Three coupled substitutions, namely, [Al]${Mg}$-[Al]${Si}$, [Fe${3+}$]${Mg}$-[Fe${3+}$]$_{Si}$, and [Fe${3+}$]${Mg}$-[Al]${Si}$ have been investigated. Aggregate elastic moduli and sound velocities are successfully compared with limited experimental data available. In the case of the [Fe${3+}$]${Mg}$-[Fe${3+}$]${Si}$ substitution, the high-spin (S=5/2) to low-spin (S=1/2) crossover in [Fe${3+}$]$_{Si}$ induces a volume collapse and elastic anomalies across the transition region. However, the associated anomalies should disappear in the presence of aluminum in the most favorable substitution, i.e., [Fe${3+}$]${Mg}$-[Al]${Si}$. Calculated elastic properties along a lower mantle model geotherm suggest that the elastic behavior of bridgmanite with simultaneous substitution of Fe${2}$O$_3$ and Al${2}$O$3$ in equal proportions or with Al${2}$O$3$ in excess should be similar to that of (Mg,Fe${2+}$)SiO$_3$ bridgmanite. Excess Fe${2}$O$_3$ should produce elastic anomalies though.

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