Research/Sitter/MAGNDATA / 1.247_NiCl2.mcif

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Spin lattice of NiCl2Spin lattice of NiCl2

NiCl2

MAGNDATA entry 1.247 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹3̄¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 52 K (−221 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 9 properties
Magnetic groupCc 2/c BNS 15.90
Parent space groupR 3m No. 166
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 3/2] 1k
Cella 3.483 · b 3.483 · c 34.8 Å · α 90° · β 90° · γ 120°
Transition52 K (−221 °C)
Magnetic ionsNi
Largest moment component2.44 μB
MethodNPD, NSD, etc.

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 Cc 2/c →
Atom sites · 2 sites · CSV
siteelementxyzmambmc|m| (μB)
Ni1Ni0002.441.2202.1131
Cl1Cl000.1275

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

M. McGuire et al. Crystals (2017) · doi:10.3390/cryst7050121

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.247_NiCl2.mcif from MAGNDATA · entry page

sha256 of this copy: 3a7c63af67b94a86f2711db6b360d7b88fd01e44db7d80cfaa7e16e51296c245
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.247_NiCl2.mcif.