Research/Sitter/MAGNDATA / 1.730_Cu2MnSiS4.mcif

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Spin lattice of Cu2Mn1Si1S4Spin lattice of Cu2Mn1Si1S4

Cu2Mn1Si1S4

MAGNDATA entry 1.730 · 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 ≤ 8 K (−265 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 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 15.0524 · b 6.4237 · c 12.3634 Å · α 90° · β 90° · γ 90°
Transition8 K (−265 °C)
Measured at2 K
Magnetic ionsMn
Largest moment component3.18 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)
Cu1_1Cu0.37650.67810.089
Cu1_2Cu0.87340.32190.339
Mn1Mn00.8420.3332.251−3.184.0218
Si1Si00.17680.0935
S1S00.860.0325
S2S00.1870.259
S3_1S0.36560.6680.276
S3_2S0.88430.3320.526

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

Z. T. Messegee et al. Inorganic Chemistry (2023) · doi:10.1021/acs.inorgchem.2c03754

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.730_Cu2MnSiS4.mcif from MAGNDATA · entry page

sha256 of this copy: a6aefb3b1743e887b14329889b0032fbc9644f83fef8f55eabf6cd7564410aff
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.730_Cu2MnSiS4.mcif.