Research/Sitter/MAGNDATA / 1.475_DyNiAl4.mcif

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Spin lattice of DyNiAl4Spin lattice of DyNiAl4

DyNiAl4

MAGNDATA entry 1.475 · 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 ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 14.6 K (−259 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPA n m a BNS 62.453
Parent space groupC m c m No. 63
Spinscollinear · net moment 0 μB per cell
Propagation[0 1 0] 1k
Cella 4.0421 · b 15.323 · c 6.589 Å · α 90° · β 90° · γ 90°
Transition14.6 K (−259 °C)
Measured at4 K
Magnetic ionsDy
Largest moment component8.1 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 PA n m a →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Dy1Dy00.11930.258.1008.1
Ni1Ni00.7720.25
Al1Al00.50
Al2Al00.9290.25
Al3Al00.3120.061

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

R. White et al. Journal of Magnetism and Magnetic Materials (2019) · doi:10.1016/j.jmmm.2018.08.011

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.475_DyNiAl4.mcif from MAGNDATA · entry page

sha256 of this copy: 3fb967b958c071c3cb5f7d0d9f4ab2b88c76c1102dd710a00d5a45cce0b6367a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.475_DyNiAl4.mcif.