Research/Sitter/MAGNDATA / 0.1103_EuSc2Te4.mcif

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Spin lattice of Eu1Sc1Te4Spin lattice of Eu1Sc1Te4

Eu1Sc1Te4

MAGNDATA entry 0.1103 · 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 ≤ 5.2 K (−268 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n′ m a BNS 62.443
Point groupm′mm
Parent space groupP n m a No. 62
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 13.1054 · b 4.2065 · c 15.2802 Å · α 90° · β 90° · γ 90°
Transition5.2 K (−268 °C)
Measured at1.4 K
Magnetic ionsEu
Largest moment component6.2 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 P n′ m a →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Eu1Eu0.23830.250.672106.206.2
Te2Te0.09380.250.0738
Te3Te0.3750.250.0328
Te4Te0.29770.250.3406
Te5Te0.46840.250.7857
Sc6Sc0.08470.250.4058
Sc7Sc0.55440.250.6119

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

Seng Huat Lee et al. Adv. Funct. Mater. (2025) · doi:10.1002/adfm.202424231

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1103_EuSc2Te4.mcif from MAGNDATA · entry page

sha256 of this copy: 756505dabecea487d8f3f64255e42c3580d0d5ddf6535d8182d693c4d78d2448
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1103_EuSc2Te4.mcif.