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Metal Vacancy Ordering in an Antiperovskite Resulting in Two Modifications of Fe 2 SeO
Author(s) -
Valldor Martin,
Wright Taylor,
Fitch Andrew,
Prots Yurii
Publication year - 2016
Publication title -
angewandte chemie international edition
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 5.831
H-Index - 550
eISSN - 1521-3773
pISSN - 1433-7851
DOI - 10.1002/anie.201603920
Subject(s) - crystallography , tetragonal crystal system , materials science , vacancy defect , crystal structure , lattice (music) , metal , atom (system on chip) , phase (matter) , chemistry , metallurgy , physics , organic chemistry , acoustics , computer science , embedded system
Small, red Fe 2 SeO single crystals in two modifications were obtained from a CsCl flux. The metastable α‐phase is pseudo‐tetragonal (Cmce, a =16.4492(8) Å, b =11.1392(4) Å, c =11.1392(4) Å), whereas the β‐phase is trigonal (P3 1 , a =9.8349(4) Å, c =6.9591(4) Å)) and thermodynamically stable within a narrow temperature range. Both crystal structures were solved from twinned specimens. The enantiomers of the β‐phase appear as racemic mixtures. Selenium and oxygen form two individual interpenetrating primitive cubic lattices, giving a bcc packing. A quasi‐octahedrally coordinated iron atom is found close to the center of each surface of the selenium sublattice. The difference between the α‐ and β‐phases is the distribution of iron at 2/3 of the surfaces. α‐ and β‐Fe 2 SeO are comparable with metal‐vacancy‐ordered antiperovskites. Each Fe/O lattice can also be described in terms of vertex‐sharing OFe 4 tetrahedra, with a crystal structure similar to that of an antisilicate. Iron is divalent and has a high‐spin d 6 ( S =2) configuration. The β‐phase exhibits magnetoelectric coupling.