Research/Sitter/MAGNDATA / 0.81_U2Pd2Sn.mcif

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Spin lattice of U2Pd2SnSpin lattice of U2Pd2Sn

U2Pd2Sn

MAGNDATA entry 0.81 · 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 ≤ 41 K (−232 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 4′/m′ b m′ BNS 127.394
Point group4′/m′m′m
Parent space groupP 4/m b m No. 127
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 7.595 · b 7.595 · c 3.799 Å · α 90° · β 90° · γ 90°
Transition41 K (−232 °C)
Measured at10 K
Magnetic ionsU
Largest moment component1.34 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 4′/m′ b m′ →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Sn1Sn000
Pd1Pd0.6330.1330
U1U0.1720.6720.51.341.3401.895

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. Purwanto et al. PHYSICAL REVIEW B (1994) · doi:10.1103/PhysRevB.50.6792

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.81_U2Pd2Sn.mcif from MAGNDATA · entry page

sha256 of this copy: 5490ef1a42aa345d108246a975a0a5503dd62fba46698678c27319c87d9d7301
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.81_U2Pd2Sn.mcif.