Spin Crossover and the Magnetic P–T Phase Diagram of Hematite at High Hydrostatic Pressures and Cryogenic Temperatures
- Authors: Gavriliuk A.G.1,2,3, Struzhkin V.V.4, Mironovich A.A.2, Lyubutin I.S.1, Troyan I.A.1,2,3, Chow P.5, Xiao Y.5
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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
- High Pressure Collaborative Access Team, Geophysical Laboratory
- Issue: Vol 107, No 4 (2018)
- Pages: 247-253
- Section: Condensed Matter
- URL: https://ogarev-online.ru/0021-3640/article/view/160921
- DOI: https://doi.org/10.1134/S0021364018040057
- ID: 160921
Cite item
Abstract
The magnetic properties of the α-Fe2O3 hematite at a high hydrostatic pressure have been studied by synchrotron Mössbauer spectroscopy (nuclear forward scattering (NFS)) on iron nuclei. Time-domain NFS spectra of hematite have been measured in a diamond anvil cell in the pressure range of 0–72 GPa and the temperature range of 36–300 K in order to study the magnetic properties at a phase transition near a critical pressure of ~50 GPa. In addition, Raman spectra at room temperature have been studied in the pressure range of 0–77 GPa. Neon has been used as a pressure-transmitting medium. The appearance of an intermediate electronic state has been revealed at a pressure of ~48 GPa. This state is probably related to the spin crossover in Fe3+ ions at their transition from the high-spin state (HS, S = 5/2) to a low-spin one (LS, S = 1/2). It has been found that the transient pressure range of the HS–LS crossover is extended from 48 to 55 GPa and is almost independent of the temperature. This surprising result differs fundamentally from other cases of the spin crossover in Fe3+ ions observed in other crystals based on iron oxides. The transition region of spin crossover appears because of thermal fluctuations between HS and LS states in the critical pressure range and is significantly narrowed at cooling because of the suppression of thermal excitations. The magnetic P–T phase diagram of α-Fe2O3 at high pressures and low temperatures in the spin crossover region has been constructed according to the results of measurements.
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
I. A. Troyan
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
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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