Research/Sitter/MAGNDATA / 0.805_DyBaCuO5.mcif

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Spin lattice of Dy2BaCuO5Spin lattice of Dy2BaCuO5

Dy2BaCuO5

MAGNDATA entry 0.805 · 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 ≤ 10.7 K (−262 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n m′ a BNS 62.444
Point groupm′m m
Parent space groupP n m a No. 62
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 12.19972 · b 5.67326 · c 7.13905 Å · α 90° · β 90° · γ 90°
Transition10.7 K (−262 °C)
Measured at1.5 K
Magnetic ionsCu, Dy
Largest moment component9.669 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 · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Dy1Dy0.28880.250.88268.6220−1.9228.8336
Dy2Dy0.07470.250.60280.55909.6699.6851
Ba1Ba−0.09150.250.0727
Cu1Cu0.65990.250.28880.5280−0.3630.6407
O1O0.56580.00980.1674
O2O0.77140.49460.3536
O3O0.10140.25−0.0842

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

P. Yanda et al. PHYSICAL REVIEW B (2021) · doi:10.1103/PhysRevB.104.144401

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.805_DyBaCuO5.mcif from MAGNDATA · entry page

sha256 of this copy: 6dba10fb13a0327cf441fa5ca5128e1ab94a4b93bd6d3865809f18c1c00a1f34
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.805_DyBaCuO5.mcif.