Research/Sitter/MAGNDATA / 1.733_Cu2MnGeS4.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Cu2Mn1Ge1S4Spin lattice of Cu2Mn1Ge1S4

Cu2Mn1Ge1S4

MAGNDATA entry 1.733 · 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).
Structure · 10 properties
Magnetic groupPa c BNS 7.27
Point groupm1′
Parent space groupP m n 21 No. 31
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 15.22 · b 6.5 · c 12.36 Å · α 90° · β 90° · γ 90°
Measured at4.2 K
Magnetic ionsMn
Largest moment component3.3 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 Pa c →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Ge1Ge00.6670.1875
Mn1Mn00.3330.4375−0.93.32.64.2965
Cu1_1Cu0.1250.1670.1875
Cu1_2Cu0.1250.8330.4375
S1S00.3330.25
S2S00.6670
S3_1S0.1250.1670
S3_2S0.1250.8330.25

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

J. Allemand et al. Bull. Soc. fr. Mineral. (1970) · doi:10.3406/bulmi.1970.6446

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.733_Cu2MnGeS4.mcif from MAGNDATA · entry page

sha256 of this copy: dfbd79a6820e7044c522cc18e2f16f998fb6596ff59a2034ce571e37d3ed71f1
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.733_Cu2MnGeS4.mcif.