Stability of fcc phase FeH to 137 GPa
We examined the crystal structure of FeHX (X∼1) (FeH hereafter) at high pressure and temperature by X-ray diffraction up to 137 GPa. Results show that FeH adopts a face-centered cubic (fcc) structure at pressures of 43 to 137 GPa and temperatures of ∼1000 to 2000 K. Our study revises a phase diagram...
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Published in | The American mineralogist Vol. 105; no. 6; pp. 917 - 921 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
Published |
Washington
Mineralogical Society of America
01.06.2020
Walter de Gruyter GmbH |
Subjects | |
Online Access | Get full text |
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Summary: | We examined the crystal structure of FeHX (X∼1) (FeH hereafter) at high pressure and temperature by X-ray diffraction up to 137 GPa. Results show that FeH adopts a face-centered cubic (fcc) structure at pressures of 43 to 137 GPa and temperatures of ∼1000 to 2000 K. Our study revises a phase diagram of stoichiometric FeH in which fcc has a wider-than-expected stability field at high pressure and temperature. Based on our findings, the FeH end-member of the Fe-FeH system is expected to be stable in the fcc structure at the P-T conditions of the Earth's core, rather than in the double-hexagonal close packed (dhcp) structure as previously reported. We compared the experimentally determined unit-cell volumes of FeH with those from ab initio calculations. Additionally, we observed a change in compressibility at ∼60 GPa, which could be attributed to a magnetic transition - an interpretation supported by our ab initio computations. |
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ISSN: | 0003-004X 1945-3027 |
DOI: | 10.2138/am-2020-7153 |