Research/Sitter/MAGNDATA / 0.990_HoFeO3.mcif

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Spin lattice of Ho1Fe1O3Spin lattice of Ho1Fe1O3

Ho1Fe1O3

MAGNDATA entry 0.990 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 6.5 K (−267 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n′ m′ a BNS 62.446
Point groupm′m′m
Parent space groupP b n m No. 62
Spinsnoncoplanar · net moment 13.6 μB per cell
Propagation[0 0 0] 1k
Cella 5.2779 · b 5.5873 · c 7.6011 Å · α 90° · β 90° · γ 90°
Transition6.5 K (−267 °C)
Measured at1.25 K
Magnetic ionsFe, Ho
Largest moment component6.68 μB
MethodNPD

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)
Ho1Ho0.4810.43220.753.4−6.6807.4955
Fe1Fe0.500004.64.6
O1O0.60560.04080.75
O2O0.69360.30870.0578

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

W. C. Koehler et al. Physical Review (1960) · doi:10.1103/PhysRev.118.58

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.990_HoFeO3.mcif from MAGNDATA · entry page

sha256 of this copy: b8a1ca2895c9d91b2481d9b719a086761533f44ffa137acabd63a6d3f2bf8b47
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.990_HoFeO3.mcif.