Research/Sitter/MAGNDATA / 1.336_Tb2Pd2.05Sn0.95.mcif

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Spin lattice of Tb2Pd2.05Sn0.95Spin lattice of Tb2Pd2.05Sn0.95

Tb2Pd2.05Sn0.95

MAGNDATA entry 1.336 · 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 ≤ 20.8 K (−252 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPb n m a BNS 62.451
Parent space groupP 4/m b m No. 127
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 7.6333 · b 7.6333 · c 7.4748 Å · α 90° · β 90° · γ 90°
Transition20.8 K (−252 °C)
Measured at1.5 K
Magnetic ionsTb
Largest moment component6.15 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 Pb n m a →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb0.17470.67470.256.156.1508.6974
Pd1Pd0.37260.87260
Sn1Sn000
Pd2Pd000.13

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

D. Laffargue et al. Journal of Alloys and Compounds (1997) · doi:10.1016/S0925-8388(97)00385-X

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.336_Tb2Pd2.05Sn0.95.mcif from MAGNDATA · entry page

sha256 of this copy: 04b9e63911e76234231b95f65e0d895381466ced316779a6fb52cfe7b4339d67
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.336_Tb2Pd2.05Sn0.95.mcif.