Research/Sitter/MAGNDATA / 0.842_DyAlO3.mcif

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Spin lattice of Dy1Al1O3Spin lattice of Dy1Al1O3

Dy1Al1O3

MAGNDATA entry 0.842 · 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 ≤ 3.5 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n′ m′ a′ BNS 62.449
Point groupm′m′m′
Parent space groupP b n m No. 62
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.21 · b 5.31 · c 7.4 Å · α 90° · β 90° · γ 90°
Transition3.48 K (−270 °C)
Measured at1.5 K
Magnetic ionsDy
Largest moment component7.2 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 P n′ m′ a′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Dy1Dy−0.0070.050.254.67.208.544
Al1Al0.500
O1O0.0520.4740.25
O2O−0.3020.2830.053

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. Bidaux et al. J. Phys. France (1968) · doi:10.1051/jphys:01968002902-3022000

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.842_DyAlO3.mcif from MAGNDATA · entry page

sha256 of this copy: 5299a776a2ca4687f67afeb7360292e6e1f7e0f7aac1e418c8a72bc068e7f5ff
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.842_DyAlO3.mcif.