Research/Sitter/MAGNDATA / 0.993_HoFeO3.mcif

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Spin lattice of Ho1Fe1O3Spin lattice of Ho1Fe1O3

Ho1Fe1O3

MAGNDATA entry 0.993 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
Structure · 10 properties
Magnetic groupP n′ m a′ BNS 62.448
Point groupm′m′m
Parent space groupP n m a No. 62
Spinscoplanar · net moment 2.8 μB per cell
Propagation[0 0 0] 1k
Cella 5.5825 · b 7.5845 · c 5.268 Å · α 90° · β 90° · γ 90°
Measured at60 K
Magnetic ionsFe, Ho
Largest moment component4.23 μB
MethodNSD

Symmetry

Stereogram of the magnetic point group: each operation applied to one direction. Filled = upper hemisphere, ring = lower; red operations include time reversal. Lines are mirrors; polygons are 2/3/4/6-fold axes; the centre ring is inversion.

Every structure in P n′ m a′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho0.06930.250.979
Fe1Fe000.500.74.234.2875
O1O0.4450.250.097
O2O0.3190.060.697

Moment components are along the crystal axes a, b, c (μB), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

A.K. Ovsianikov et al. Journal of Magnetism and Magnetic Materials (2022) · doi:10.1016/j.jmmm.2022.169431

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.993_HoFeO3.mcif from MAGNDATA · entry page

sha256 of this copy: 6add856034d23954b0f00f32663a43cd67af19ea278d97c0d5568fc1b85863e8
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.993_HoFeO3.mcif.