Research/Sitter/MAGNDATA / 0.960_Fe2TeO6.mcif

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Spin lattice of Fe2Te1O6Spin lattice of Fe2Te1O6

Fe2Te1O6

MAGNDATA entry 0.960 · 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 ¹4/¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 218.5 K (−55 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 42/m′ n′ m′ BNS 136.503
Point group4/m′m′m′
Parent space groupP 42/m n m No. 136
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 4.601 · b 4.601 · c 9.087 Å · α 90° · β 90° · γ 90°
Transition218.5 K (−55 °C)
Measured at4.2 K
Magnetic ionsFe
Largest moment component2.36 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 42/m′ n′ m′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe000.3335002.362.36
Te1Te000
O1O0.2990.2990
O2O0.3070.3070.3355

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

M. C. Montmory et al. Solid State Communications (1968) · doi:10.1016/0038-1098(68)90113-0

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.960_Fe2TeO6.mcif from MAGNDATA · entry page

sha256 of this copy: 04b0f27b9f3ff478a875f933d7a0e8bcf396ea8ec25c760a801c1dd161499a75
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.960_Fe2TeO6.mcif.