Stability and equation of state of post-aragonite BaCO3

Joshua P. Townsend, Yun Yuan Chang, Xiaoting Lou, Miguel Merino, Scott J. Kirklin, Jeff W. Doak, Ahmed Issa, Chris Wolverton, Sergey N. Tkachev, Przemyslaw Dera, Steven D. Jacobsen

Research output: Contribution to journalArticlepeer-review

19 Scopus citations

Abstract

At ambient conditions, witherite is the stable form of BaCO3 and has the aragonite structure with space group Pmcn. Above ~10 GPa, BaCO3 adopts a post-aragonite structure with space group Pmmn. High-pressure and high-temperature synchrotron X-ray diffraction experiments were used to study the stability and equation of state of post-aragonite BaCO3, which remained stable to the highest experimental P-T conditions of 150 GPa and 2,000 K. We obtained a bulk modulus K0 = 88(2) GPa with K′ = 4.8(3) and V0 = 128.1(5) Å3 using a third-order Birch-Murnaghan fit to the 300 K experimental data. We also carried out density functional theory (DFT) calculations of enthalpy (H) of two structures of BaCO3 relative to the enthalpy of the post-aragonite phase. In agreement with previous studies and the current experiments, the calculations show aragonite to post-aragonite phase transitions at ~8 GPa. We also tested a potential high-pressure post-post-aragonite structure (space group C2221) featuring four-fold coordination of oxygen around carbon. In agreement with previous DFT studies, ΔH between the C2221 structure and post-aragonite (Pmmn) decreases with pressure, but the Pmmn structure remains energetically favorable to pressures greater than 200 GPa. We conclude that post-post-aragonite phase transformations of carbonates do not follow systematic trends observed for post-aragonite transitions governed solely by the ionic radii of their metal cations.

Original languageEnglish (US)
Pages (from-to)447-453
Number of pages7
JournalPhysics and Chemistry of Minerals
Volume40
Issue number5
DOIs
StatePublished - May 2013

Funding

This research was supported by the NSF EAR-074787 (CAREER), the Carnegie/DOE Alliance Center (CDAC), and by the David and Lucile Packard Foundation to SDJ. Portions of this work were performed at GeoSoilEnviroCARS (GSECARS), Sector 13, Advanced Photon Source (APS), Argonne National Laboratory. GSECARS is supported by the NSF EAR-0622171 and Department of Energy DE-FG02-94ER14466. Use of the APS was supported by the DOE Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357. This research was partially supported by COMPRES, the Consortium for Materials Properties Research in Earth Sciences under NSF Cooperative Agreement EAR 11-57758. SK was supported by the Center for Electrical Energy Storage: Tailored Interfaces, an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science and Office of Basic Sciences. AI was supported by the Ford-Boeing-Northwestern (FBN) alliance, award no. 81132882. JWD was supported by the Revolutionary Materials for Solid State EnergyConversion, an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciencesunder Award Number DE-SC00010543.

Keywords

  • Carbonates
  • Equation of state
  • High pressure

ASJC Scopus subject areas

  • General Materials Science
  • Geochemistry and Petrology

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