Research/Sitter/MAGNDATA / 0.1077_Cu2(MoO4)(SeO3).mcif

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Spin lattice of Cu2Mo1Se1O7Spin lattice of Cu2Mo1Se1O7

Cu2Mo1Se1O7

MAGNDATA entry 0.1077 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 23.6 K (−250 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21′/c BNS 14.77
Point group2′/m
Parent space groupP 21/c No. 14
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 8.104 · b 8.991 · c 8.386 Å · α 90° · β 104.74° · γ 90°
Transition23.6 K (−250 °C)
Measured at4 K
Magnetic ionsCu
Largest moment component0.73 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 P 21′/c →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Cu1Cu0.31690.99290.38010.440.180.690.74
Cu2Cu0.31660.99330.02760.0600.730.7171
Mo1Mo0.12180.28640.162
Se1Se0.32180.67290.2029
O1O0.3720.85580.212
O2O0.4350.61310.3887
O3O0.4380.60870.078
O4O0.21230.10780.175
O5O0.1730.39070.0004
O6O00.2710.108
O7O0.18750.39950.341

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

Pharit Piyawongwatthana et al. PHYSICAL REVIEW B (2024) · doi:10.1103/PhysRevB.109.224420

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1077_Cu2(MoO4)(SeO3).mcif from MAGNDATA · entry page

sha256 of this copy: ea5cf238ad019829e84cef3b350d77b032fe19dd10cf7d12b1650925c4a0d596
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1077_Cu2(MoO4)(SeO3).mcif.