Research/Sitter/MAGNDATA / 1.0.60_Ce2SnS5.mcif

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Spin lattice of Ce2Sn1S5Spin lattice of Ce2Sn1S5

Ce2Sn1S5

MAGNDATA entry 1.0.60 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 1.2 K (−272 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP b′ a′ m′ BNS 55.359
Point groupm′m′m′
Parent space groupP b a m No. 55
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 23.5689 · b 11.2219 · c 3.9563 Å · α 90° · β 90° · γ 90°
Transition1.2 K (−272 °C)
Measured at0.3 K
Magnetic ionsCe
Largest moment component1.25 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 b′ a′ m′ →
Atom sites · 13 sites · CSV
siteelementxyzmambmc|m| (μB)
Ce1_1Ce0.02320.33080.50.21.2501.2659
Ce1_2Ce0.97680.66920.50.84−0.94601.2651
Ce1_3Ce0.14340.83080.5−0.35−1.21501.2644
Sn1_1Sn000
Sn1_2Sn0.16670.50
S1_1S0.06220.07220.5
S1_2S0.93780.92770.5
S1_3S0.10450.57230.5
S2_1S0.11770.29880
S2_2S0.88230.70130
S2_3S0.0490.79870
S3_1S00.50
S3_2S0.166700

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

Maximilien F. Debbas et al. PHYSICAL REVIEW B (2025) · doi:10.1103/xv8k-812w

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.0.60_Ce2SnS5.mcif from MAGNDATA · entry page

sha256 of this copy: 1ee19cedab95a0f3f11d093d5cd28a1d03d6b5a1f0397d208ae1bc49356df070
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.60_Ce2SnS5.mcif.