Research/Sitter/MAGNDATA / 1.51_Cs2CoCl4.mcif

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Spin lattice of Cs2CoCl4Spin lattice of Cs2CoCl4

Cs2CoCl4

MAGNDATA entry 1.51 · source
p-wave magnet
Coplanar spins, no net moment, and a translation that reverses every spin: spin splitting that is odd in momentum (p-wave).
ordered ≤ 0.2 K (−273 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPa 21 BNS 4.10
Point group21′
Parent space groupP n m a No. 62
Spinscoplanar · net moment 0 μB per cell
Propagation[0 1/2 1/2] 1k
Cella 9.72 · b 14.626 · c 25.644 Å · α 90° · β 90° · γ 90°
Transition0.217 K (−273 °C)
Measured at0.08 K
Magnetic ionsCo
Largest moment component1.6 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 Pa 21 →
Atom sites · 14 sites · CSV
siteelementxyzmambmc|m| (μB)
Cs1_1Cs0.35990.1250.0504
Cs1_2Cs0.6401−0.125−0.0504
Cs2_1Cs0.02220.125−0.0882
Cs2_2Cs−0.0222−0.1250.0882
Co1_1Co0.76490.1250.03890−1.6−0.41.6492
Co1_2Co0.2351−0.125−0.03890−1.60.41.6492
Cl1_1Cl−0.00370.1250.05
Cl1_2Cl0.00370.3750.45
Cl2_1Cl0.68770.1250.4556
Cl2_2Cl0.31230.3750.0444
Cl31_1Cl0.6740.25090.0764
Cl31_2Cl0.326−0.2509−0.0764
Cl32_1Cl0.8260.24910.3264
Cl32_2Cl0.1740.25090.1736

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. Kenzelmann et al. PHYSICAL REVIEW B (2002) · doi:10.1103/physrevb.65.144432

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.51_Cs2CoCl4.mcif from MAGNDATA · entry page

sha256 of this copy: ca7b51be9d2f8046782c8d04e73b58c0aa1175ae24f0fa31b5040b9263b91664
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.51_Cs2CoCl4.mcif.