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American Mineralogist; May 2008; v. 93; no. 5-6; p. 745-750; DOI: 10.2138/am.2008.2428
© 2008 Mineralogical Society of America
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Thermal equation of state of CaGeO3 perovskite

Wei Liu1,*, Jennifer Kung2, Liping Wang1 and Baosheng Li1

1 Mineral Physics Institute, Stony Brook University, Stony Brook, New York 11794, U.S.A.
2 Department of Earth Sciences, National Cheng-Kung University, Tainan 70101, Taiwan

Correspondence: * E-mail: weiliu3{at}notes.cc.sunysb.edu

Pressure-volume-temperature data have been obtained for CaGeO3 perovskite up to 9.6 GPa and 1100 K using a cubic anvil, DIA-type high-pressure apparatus in conjunction with synchrotron X-ray diffraction. The data were analyzed using Birch-Murnaghan equation of state and thermal pressure approach with the bulk modulus at ambient pressure, KT0, and its pressure derivative, K'T0, constrained by previous measurements. A fit of the unit-cell volume data to the high-temperature Birch-Murnaghan (HTBM) equation of state gives ({partial}KT/{partial}T)P = –0.025 ± 0.015 GPa/K, a = 1.047 ± 0.356 x 10–5/K, and b = 3.282 ± 0.735 x 10–8/K2 for the thermal expansion {alpha} expressed by a + bT. The thermal pressure approach yields {alpha}KT = 4.04 ± 0.37 x 10–3 GPa/K and ({partial}2P/{partial}T2)V = 6.17 ± 1.28 x 10–6 GPa/K2. The energy dispersive X-ray diffraction data reveal no indication of a structural phase transition over the P-T range of the current experiment. A systematic relationship, KS0 = 6720/V(molar) – 13.07 GPa, has been established based on these isostructural analogues, which predicts KS0 = 261(15) for MgSiO3 perovskite and 225(8) for CaSiO3 perovskite, respectively.

Key Words: CaGeO3 perovskite • equation of state • thermal pressure • high pressure and high temperature • X-ray diffraction







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