Low-Temperature P–T Phase Diagram of the (Mg, Fe)SiO3 Perovskite
- Authors: Gavriliuk A.G.1,2,3, Struzhkin V.V.4, Mironovich A.A.2, Lyubutin I.S.1, Lin J.F.5, Ivanova A.G.1,2, Chow P.6, Xiao Y.6
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Affiliations:
- Shubnikov Institute of Crystallography, Federal Research Center Crystallography and Photonics
- Institute for Nuclear Research
- Immanuel Kant Baltic Federal University
- Geophysical Laboratory
- Department of Geological Sciences, Jackson School of Geosciences
- High Pressure Collaborative Access Team, Geophysical Laboratory
- Issue: Vol 107, No 11 (2018)
- Pages: 705-712
- Section: Condensed Matter
- URL: https://ogarev-online.ru/0021-3640/article/view/161115
- DOI: https://doi.org/10.1134/S0021364018110085
- ID: 161115
Cite item
Abstract
The electron spin states of iron in minerals of the Earth’s mantle at high pressures mostly determine the physicochemical properties of deep layers of the Earth and are of great interest not only for geophysics but also for fundamental physics of strongly correlated electron systems. In this work, using Raman and synchrotron Mössbauer nuclear forward scattering (NFS) spectroscopies, iron-containing magnesium–silicate perovskite (Mg, Fe)SiO3 (10% Fe) has been studied in the cryogenic temperature range of 35–300 K and at high pressures up to 48 GPa, which are created in diamond anvil cells. The analysis of NFS spectra has indicated that iron ions are in a nonmagnetic (para- or diamagnetic) state in the entire region of temperatures and pressures and the electronic properties can be controlled by means of the quadrupole splitting parameter. It has been found that an increase in the pressure and a decrease in the temperature are accompanied by a significant increase in the parameter Δ from 2 mm/s to ~4 mm/s, which indicates that the electronic state of Fe2+ ions changes. The maximum Δ value has been observed at P > 20 GPa, but the pressure behavior of a transition strongly depends on the temperature. Possible mechanisms of the transition have been discussed.
About the authors
A. G. Gavriliuk
Shubnikov Institute of Crystallography, Federal Research Center Crystallography and Photonics; Institute for Nuclear Research; Immanuel Kant Baltic Federal University
Email: lyubutinig@mail.ru
Russian Federation, Moscow, 119333; Moscow, 117312; Kaliningrad, 236041
V. V. Struzhkin
Geophysical Laboratory
Email: lyubutinig@mail.ru
United States, Washington, DC, 20015
A. A. Mironovich
Institute for Nuclear Research
Email: lyubutinig@mail.ru
Russian Federation, Moscow, 117312
I. S. Lyubutin
Shubnikov Institute of Crystallography, Federal Research Center Crystallography and Photonics
Author for correspondence.
Email: lyubutinig@mail.ru
Russian Federation, Moscow, 119333
J. F. Lin
Department of Geological Sciences, Jackson School of Geosciences
Email: lyubutinig@mail.ru
United States, Austin, TX, 78712
A. G. Ivanova
Shubnikov Institute of Crystallography, Federal Research Center Crystallography and Photonics; Institute for Nuclear Research
Email: lyubutinig@mail.ru
Russian Federation, Moscow, 119333; Moscow, 117312
P. Chow
High Pressure Collaborative Access Team, Geophysical Laboratory
Email: lyubutinig@mail.ru
United States, Argonne, IL, 60439
Y. Xiao
High Pressure Collaborative Access Team, Geophysical Laboratory
Email: lyubutinig@mail.ru
United States, Argonne, IL, 60439
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