Postaragonite phases of CaCO3 at lower mantle pressures

Dean Smith, Keith V. Lawler, Miguel Martinez-Canales, Austin W. Daykin, Zachary Fussell, G. Alexander Smith, Christian Childs, Jesse S. Smith, Chris J. Pickard, and Ashkan Salamat
Phys. Rev. Materials 2, 013605 – Published 31 January 2018

Abstract

The stability, structure, and properties of carbonate minerals at lower mantle conditions have significant impact on our understanding of the global carbon cycle and the composition of the interior of the Earth. In recent years there has been significant interest in the behavior of carbonates at lower mantle conditions, specifically in their carbon hybridization, which has relevance for the storage of carbon within the deep mantle. Using high-pressure synchrotron x-ray diffraction in a diamond anvil cell coupled with direct laser heating of CaCO3 using a CO2 laser, we identify a crystalline phase of the material above 40 GPa—corresponding to a lower mantle depth of around 1000 km—which has first been predicted by ab initio structure predictions. The observed sp2 carbon hybridized species at 40 GPa is monoclinic with P21/c symmetry and is stable up to 50 GPa, above which it transforms into a structure which cannot be indexed by existing known phases. A combination of ab initio random structure search (AIRSS) and quasiharmonic approximation (QHA) calculations are used to re-explore the relative phase stabilities of the rich phase diagram of CaCO3. Nudged elastic band (NEB) calculations are used to investigate the reaction mechanisms between relevant crystal phases of CaCO3 and we postulate that the mineral is capable of undergoing sp2sp3 hybridization change purely in the P21/c structure—forgoing the accepted postaragonite Pmmn structure.

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  • Received 7 September 2017
  • Revised 27 November 2017

DOI:https://doi.org/10.1103/PhysRevMaterials.2.013605

©2018 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Dean Smith1, Keith V. Lawler2, Miguel Martinez-Canales3, Austin W. Daykin1, Zachary Fussell1, G. Alexander Smith2, Christian Childs1, Jesse S. Smith4, Chris J. Pickard5,6, and Ashkan Salamat1,*

  • 1Department of Physics and Astronomy and HiPSEC, University of Nevada Las Vegas, Las Vegas, Nevada 89154, USA
  • 2Department of Chemistry and Biochemistry and HiPSEC, University of Nevada Las Vegas, Las Vegas, Nevada 89154, USA
  • 3Scottish Universities Physics Alliance (SUPA), School of Physics and Astronomy and Centre for Science at Extreme Conditions, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom
  • 4High Pressure Collaborative Access Team, Geophysical Laboratory, Carnegie Institution of Washington, Argonne, Illinois 60439, USA
  • 5Department of Materials Science and Metallurgy, University of Cambridge, Cambridge CB3 0FS, United Kingdom
  • 6Advanced Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan

  • *Author to whom correspondence should be addressed: salamat@physics.unlv.edu

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Vol. 2, Iss. 1 — January 2018

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