Research/Sitter/MAGNDATA / 1.1.77_NiBr2.mcif

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Spin lattice of NiBr2Spin lattice of NiBr2

NiBr2

MAGNDATA entry 1.1.77 · source
incommensurate spiral
Incommensurate: the magnetic pattern repeats every so many cells, but not a whole number of them, so it never lines up with the crystal lattice. Here it's a spiral: the spin direction rotates as you move along.
ordered ≤ 22.8 K (−250 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupRm1′(ααγ)0s
Point groupm1′
Parent space groupR 3m No. 166
Repeats every0.67 cells along c (not a whole number: that's what incommensurate means)
Propagation[0.027 0.027 1.5] 1k
Cella 3.723 · b 3.723 · c 18.34 Å · α 90° · β 90° · γ 120°
Transition22.8 K (−250 °C)
Measured at4.2 K
Magnetic ionsNi
Largest moment component2 μB
MethodNSD and NPD

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 Rm1′(ααγ)0s →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Ni1Ni000
Br1_1Br000.255
Br1_2Br00−0.255

Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.

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. Adam et al. Solid State Communications (1980) · doi:10.1016/0038-1098(80)90757-7

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.1.77_NiBr2.mcif from MAGNDATA · entry page

sha256 of this copy: d8d0798c6f5753f9bb34f0d6bfc5b32c1d4b8f9a44da5029ebb241d6695539a2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.77_NiBr2.mcif.