Research/Sitter/MAGNDATA / 0.905_Tb2PdGe6.mcif

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Spin lattice of Tb2Pd1Ge6Spin lattice of Tb2Pd1Ge6

Tb2Pd1Ge6

MAGNDATA entry 0.905 · 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 ≤ 48 K (−225 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC m′ c a BNS 64.471
Point groupm′mm
Parent space groupC m c e No. 64
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 8.1861 · b 8.0548 · c 21.6022 Å · α 90° · β 90° · γ 90°
Transition48 K (−225 °C)
Measured at1.9 K
Magnetic ionsTb
Largest moment component8.32 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 C m′ c a →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb0.25560.3810.08132.298.3208.6294
Pd1Pd00.14990.1448
Ge1Ge0.27860.11510.1913
Ge2Ge00.10450.4617
Ge3Ge00.13210.0292
Ge4Ge00.3540.3099
Ge5Ge00.40040.1997

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

B. Penc et al. Journal of Magnetism and Magnetic Materials (2020) · doi:10.1016/j.jmmm.2020.167152

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.905_Tb2PdGe6.mcif from MAGNDATA · entry page

sha256 of this copy: e6792579db0271b999a4dff14533bf59631bd4cc39b0216a316b83bdae8188d7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.905_Tb2PdGe6.mcif.