Research/Sitter/MAGNDATA / 0.1123_Li2CoCl4.mcif

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Spin lattice of Cl4CoLi2Spin lattice of Cl4CoLi2

Cl4CoLi2

MAGNDATA entry 0.1123 · source
s-wave ferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Spin group ¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
Structure · 10 properties
Magnetic groupC m′ m′ m BNS 65.485
Point groupm′m′m
Parent space groupC m m m No. 65
Spinscollinear · net moment 4.1 μB per cell
Propagation[0 0 0] 1k
Cella 7.167196 · b 10.234643 · c 3.609807 Å · α 90° · β 90° · γ 90°
Measured at1.5 K
Magnetic ionsCo
Largest moment component2.05 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 C m′ m′ m →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Li1Li0.250.250.5
Co1Co000002.052.05
Cl1Cl0.237300.5
Cl2Cl00.23810

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

Zachary W. Riedel et al. PHYSICAL REVIEW B (2025) · doi:10.1103/tqwb-v5r2

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1123_Li2CoCl4.mcif from MAGNDATA · entry page

sha256 of this copy: 3d2f393c827d8014f087cf4e02a80bc8277b1f6963f09683bdc6237860db3e98
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1123_Li2CoCl4.mcif.