Research/Sitter/MAGNDATA / 1.416_Tb2O2S.mcif

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Spin lattice of Tb2O2SSpin lattice of Tb2O2S

Tb2O2S

MAGNDATA entry 1.416 · 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 ≤ 6 K (−267 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupCc 2/c BNS 15.90
Parent space groupP 3 m 1 No. 164
Spinscollinear · net moment 0 μB per cell
Propagation[0 1/2 1/2] 1k
Cella 3.814 · b 6.606 · c 13.232 Å · α 90° · β 90° · γ 90°
Transition6 K (−267 °C)
Measured at4.2 K
Magnetic ionsTb
Largest moment component5.3 μB
MethodNSD

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 Cc 2/c →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb00.33330.14105.34.97.218
S1S000
O1O00.33330.315

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

Y. Abbas et al. Physica B+C (1977) · doi:10.1016/0378-4363(77)90251-0

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.416_Tb2O2S.mcif from MAGNDATA · entry page

sha256 of this copy: 6faa829345b1ce3a96bd71a53030633c731fa1bf1713441a70f1b248e54263b2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.416_Tb2O2S.mcif.