Research/Sitter/MAGNDATA / 1.750_HoSbTe.mcif

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Spin lattice of Ho1Sb1Te1Spin lattice of Ho1Sb1Te1

Ho1Sb1Te1

MAGNDATA entry 1.750 · 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 ¹2/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 3 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPa 21/m BNS 11.55
Point group2/m1′
Parent space groupP 4/n m m No. 129
Spinscollinear · net moment 0 μB per cell
Propagation[1/2 0 1/4] 1k
Cella 8.43764 · b 4.21882 · c 18.7343 Å · α 90° · β 103.0091° · γ 90°
Transition3 K (−270 °C)
Measured at2.5 K
Magnetic ionsHo
Largest moment component4.985 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 Pa 21/m →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1_1Ho0.18110.250.112204.98504.985
Ho1_2Ho0.43110.250.612204.98504.985
Sb1_1Sb0.750.250.75
Sb1_2Sb00.250.25
Te2_1Te0.09450.25−0.0611
Te2_2Te0.34440.250.4389

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

I. Plokhikh et al. Inorg. Chem. (2022) · doi:10.1021/acs.inorgchem.2c01711

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.750_HoSbTe.mcif from MAGNDATA · entry page

sha256 of this copy: 54f0bddad7436ee0377a638b7403f3c172720d4408bb931d3eeb7070e8d93df1
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.750_HoSbTe.mcif.