Research/Sitter/MAGNDATA / 1.697_Tb5Pd2In4.mcif

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Spin lattice of Tb5Pd2In4Spin lattice of Tb5Pd2In4

Tb5Pd2In4

MAGNDATA entry 1.697 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 60 K (−213 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPb m c 21 BNS 26.72
Point groupmm21′
Parent space groupP b a m No. 55
Spinscollinear · net moment 0 μB per cell
Propagation[0 1/2 0] 1k
Cella 18.1642 · b 16.0076 · c 3.6467 Å · α 90° · β 90° · γ 90°
Transition60 K (−213 °C)
Measured at39.7 K
Magnetic ionsTb
Largest moment component7.4 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 m c 21 →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb000007.47.4
Tb2_1Tb0.21780.12050
Tb2_2Tb0.78220.87960
Tb3_1Tb0.420.059200077
Tb3_2Tb0.580.9408000−77
Pd1_1Pd0.30220.01160.5
Pd1_2Pd0.69780.98840.5
In1_1In0.56970.10410.5
In1_2In0.43030.89590.5
In2_1In0.85040.03780.5
In2_2In0.14960.96220.5

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

S. Baran et al. J. Alloys Compd. (2021) · doi:10.1016/j.jallcom.2021.160171

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.697_Tb5Pd2In4.mcif from MAGNDATA · entry page

sha256 of this copy: a043d853907fbdea35a608b06095a95fe818c8596f474f9cdedb21d926b01c15
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.697_Tb5Pd2In4.mcif.