T17 Frontiers in Mineral Sciences: Mineral/Melt Energetics, Mineral Surface Chemistry, Mineral Nanoscience, and High-Pressure Mineralogy I
Sunday, 18 October 2009
8:00 AM - 12:00 PM
E145
TRIVALENT CATIONS IN MANTLE SILICATE PEROVSKITE
Paper number: T17-4
Program: Technical Sessions
Time: 8:45 AM – 9:00 AM
Authors
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William J. EvansLawrence Livermore National Lab, Livermore, CA
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Sang-Heon ShimMassachusetts Institute of Technology, Cambridge, MA
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Przemyslaw DeraUniversity of Illinois at Chicago, Argonne, IL
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Vitali PrakapenkaUniversity of Illinois at Chicago, Argonne, IL
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Yuming XiaoAdvanced Photon Source, Argonne, IL
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Paul ChowAdvanced Photon Source, Argonne, IL
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Jiyong ZhaoArgonne National Lab, Argonne, IL
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Wolfgang SturhahnArgonne National Lab, Argonne, IL
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Hyunchae CynnLawrence Livermore National Lab, Livermore, CA
Abstract
Above 50 GPa, Fe3+ and Al3+ enter the perovskite structure primarily by charge-coupled substitution. When Fe3+ exists alone in perovskite, it enters both the dodecahedral and octahedral sites. With compression, Fe3+ in the octahedral site undergoes a gradual change to the low spin state, while Fe3+ in the dodecahedral site remains high spin to at least 136 GPa. The spin transition results in a low bulk modulus for perovskite below 60 GPa.
When Fe3+ exists together with Al, at low pressure the majority of Fe3+ sits in the dodecahedral site in the high spin state. However, we found a rapid increase in the low spin Fe3+ fraction in the octahedral site of perovskite at ~70 GPa. Because low spin Fe3+ is similar in size to Al3+, more Fe3+ enters the octahedral site at higher pressure, while Al3+ must enter into the dodecahedral site. Above 80 GPa, approximately half of the Fe3+ exists in the octahedral site. As a result of the site mixing, the Al-bearing perovskite has a significantly smaller volume at lowermost mantle pressures.