Research/Sitter/MAGNDATA / 0.4_NiCr2O4.mcif

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Spin lattice of NiCr2O4Spin lattice of NiCr2O4

NiCr2O4

MAGNDATA entry 0.4 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹4/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 74 K (−199 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupF d′ d′ d BNS 70.530
Point groupm′m′m
Parent space groupI 41/a m d No. 141
Spinscollinear · net moment 4.639 μB per cell
Propagation[0 0 0] 1k
Cella 5.8102 · b 5.8102 · c 8.4806 Å · α 90° · β 90° · γ 90°
Transition74 K (−199 °C)
Magnetic ionsCr, Ni
Largest moment component1.16 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 F d′ d′ d →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Ni1Ni00.250.3751.161.1601.6405
Cr1Cr000−0.99−0.9901.4001
O1O00.98210.2337

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

Tomiyasu, K. et al. J. Phys. Soc Jpn (2004)

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.4_NiCr2O4.mcif from MAGNDATA · entry page

sha256 of this copy: 9fefc02dde01d137af8613fd00142f1f4c19e60043e5de482b7a01e140bb11a0
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.4_NiCr2O4.mcif.