Research/Sitter/MAGNDATA / 0.248_TbPt0.8Cu0.2.mcif

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Spin lattice of TbPt0.8Cu0.2Spin lattice of TbPt0.8Cu0.2

TbPt0.8Cu0.2

MAGNDATA entry 0.248 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 47 K (−226 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n′ m′ a BNS 62.446
Parent space groupP n m a No. 62
Spinscoplanar · net moment 20.88 μB per cell
Propagation[0 0 0] 1k
Cella 7.0024 · b 4.4823 · c 5.5293 Å · α 90° · β 90° · γ 90°
Transition47 K (−226 °C)
Measured at1.5 K
Magnetic ionsTb
Largest moment component6.45 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 · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb0.1820.250.137−6.4505.228.2976
Pt1Pt0.0380.250.65
Cu1Cu0.0380.250.65

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. Senas et al. PHYSICAL REVIEW B (2004) · doi:10.1103/PhysRevB.70.184425

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.248_TbPt0.8Cu0.2.mcif from MAGNDATA · entry page

sha256 of this copy: 94668c57d8c96cbc313ea7ce7ecffa6422b028e535030035a3cf42b020ce451b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.248_TbPt0.8Cu0.2.mcif.