Research/Sitter/MAGNDATA / 0.163_MnPS3.mcif

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Spin lattice of MnPS3Spin lattice of MnPS3

MnPS3

MAGNDATA entry 0.163 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹2/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 78 K (−195 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC 2′/m BNS 12.60
Point group2′/m
Parent space groupC 2/m No. 12
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 6.077 · b 10.524 · c 6.796 Å · α 90° · β 107.35° · γ 90°
Transition78 K (−195 °C)
Measured at10 K
Magnetic ionsMn
Largest moment component4.6 μB
MethodNSD, Neutron polarimetry.

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 2′/m →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn00.332601.9904.64.434
P1P0.055600.1686
S1S0.759300.2497
S2S0.24380.16120.2516

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

E. Ressouche et al. PHYSICAL REVIEW B (2010) · doi:10.1103/PhysRevB.82.100408

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.163_MnPS3.mcif from MAGNDATA · entry page

sha256 of this copy: ef48ec4626199f233b68420a6a91223c1b654bb6f19d46f0b45c015f68c9d4f1
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.163_MnPS3.mcif.