High pressure dissociation of CaTiO3 perovskite into CaO and CaTi2O5

被引:2
|
作者
Truffet, B. [1 ]
Fiquet, G. [1 ]
Morard, G. [1 ,5 ]
Baron, M. A. [1 ]
Miozzi, F. [1 ,6 ]
Harmand, M. [1 ]
Ravasio, A. [2 ]
Mezouar, M. [3 ]
Guyot, F. [1 ,4 ]
机构
[1] Sorbonne Univ, Inst Mineral Phys Mat & Cosmochimie, Museum Natl Hist Nat, UMR CNRS 7590, 4 Pl Jussieu, F-75005 Paris, France
[2] Sorbonne Univ, Ecole Polytech, Lab Utilisat Lasers Intenses LULI, CNRS,CEA, Palaiseau, France
[3] European Synchrotron Radiat Facil, ESRF, Grenoble, France
[4] Inst Univ France IUF, Paris, France
[5] Univ Grenoble Alpes, Univ Savoie Mt Blanc, CNRS, IRD,Univ Gustave Eiffel,ISTerre, F-38000 Grenoble, France
[6] Carnegie Inst Sci, Earth & Planets Lab, Washington, DC USA
基金
欧洲研究理事会;
关键词
Dissociation; High-pressure; Perovskite; CaTiO3; Equation of State; X-RAY-DIFFRACTION; EQUATION-OF-STATE; TEMPERATURE HEAT-CAPACITY; PHASE-TRANSITIONS; POST-PEROVSKITE; CASIO3; PEROVSKITE; MGSIO3; SINGLE-CRYSTAL; SYSTEM; STABILITY;
D O I
10.1016/j.pepi.2022.106968
中图分类号
P3 [地球物理学]; P59 [地球化学];
学科分类号
0708 ; 070902 ;
摘要
In this study, we investigated phase transformations of CaTiO3 perovskite using x-ray diffraction at high pressure and high temperature up to 170 GPa and 4500 K in a laser-heated diamond-anvil cell. We report a high-pressure dissociation of CaTiO3 into CaO-B2 and CaTi2O5 with a monoclinic P2/m structure, instead of the expected transformation of the orthorhombic distorted perovskite structure into a post-perovskite phase. We propose that this transition may be favored by the B1 to B2 phase change of CaO at around 60 GPa. In order to provide additional information on the high pressure properties of CaTiO3 perovskite, we measured its melting temper-ature using CO2 laser heated diamond anvil cell up to 55 GPa yielding a fit of the melting curve to a Kraut-Kennedy empirical law according to: Tm (K) = 2188 * [1 + 4.23 * (Delta V/V0)]. To provide some further insight into the thermodynamic properties of CaTiO3, we determined the P-V-T equation of state of the orthorhombic mineral perovskite, fitted by using a third order Birch-Murnaghan equation of state and a Berman thermal expansion model. The fit of the data yields to K0 = 180.6(4) GPa, K ' 0 = 4 (fixed), partial differential K/ partial differential T =-0.022(1) GPa K-1, alpha 1 = 3.25(5) x 10-5 K-1, alpha 2 = 1.3(1) x 10-8 K-2
引用
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页数:11
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