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...

Full description

Saved in:
Bibliographic Details
Published inThe American mineralogist Vol. 105; no. 6; pp. 917 - 921
Main Authors Kato, Chie, Umemoto, Koichiro, Ohta, Kenji, Tagawa, Shoh, Hirose, Kei, Ohishi, Yasuo
Format Journal Article
LanguageEnglish
Published Washington Mineralogical Society of America 01.06.2020
Walter de Gruyter GmbH
Subjects
Online AccessGet full text

Cover

Loading…
More Information
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.
ISSN:0003-004X
1945-3027
DOI:10.2138/am-2020-7153