Research/Sitter/MAGNDATA / 1.0.34_RbNiCl3.mcif

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Spin lattice of RbNiCl3Spin lattice of RbNiCl3

RbNiCl3

MAGNDATA entry 1.0.34 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 11.2 K (−262 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC m′ c 21′ BNS 36.174
Parent space groupP 63/m m c No. 194
Spinscoplanar · net moment 0 μB per cell
Propagation[1/3 1/3 0] · [0 0 0] 1k
Cella 20.76 · b 20.76 · c 5.87 Å · α 90° · β 90° · γ 120°
Transition11.15 K (−262 °C)
Measured at4.5 K
Magnetic ionsNi
Largest moment component1.25 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 C m′ c 21′ →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Rb1_1Rb0.11110.22220.75
Rb1_2Rb0.11110.88890.75
Ni1_1Ni000001.251.25
Ni1_2Ni00.333301.0541.054−0.6721.25
Cl1_1Cl0.05330.10670.25
Cl1_2Cl0.05330.94670.25
Cl1_3Cl0.05330.440.25
Cl1_4Cl0.89330.280.25
Cl1_5Cl0.05330.280.25

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. B. Yelon et al. PHYSICAL REVIEW B (1972) · doi:10.1103/PhysRevB.6.204

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.0.34_RbNiCl3.mcif from MAGNDATA · entry page

sha256 of this copy: 5effec914ada402c5c105c2cc167c1f86afc214f1404d1640fbb69b8ada8f21c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.34_RbNiCl3.mcif.