Research/Sitter/MAGNDATA / 1.768_Ni2Mo3O8.mcif

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Spin lattice of Ni2Mo3O8Spin lattice of Ni2Mo3O8

Ni2Mo3O8

MAGNDATA entry 1.768 · 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 ≤ 5 K (−268 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPC n a 21 BNS 33.154
Point groupmm21′
Parent space groupP 63 m c No. 186
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 0 0] 1k
Cella 11.4976 · b 5.7488 · c 9.859 Å · α 90° · β 90° · γ 120°
Transition5 K (−268 °C)
Measured at1.5 K
Magnetic ionsNi
Largest moment component2.4 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 PC n a 21 →
Atom sites · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
Ni1Ni0.16670.66670.9744−2.4−1.2−0.952.2853
Ni2Ni0.16670.66670.53621.240.62−0.161.0857
Mo1_1Mo0.07340.85320.274
Mo1_2Mo0.85320.85320.274
O1O000.4164
O2O0.16670.66670.1713
O3_1O0.24270.51450.3909
O3_2O0.51450.51450.3909
O4_1O0.08390.83220.6576
O4_2O0.83220.83220.6576

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

P. Yadav et al. PHYSICAL REVIEW RESEARCH (2023) · doi:10.1103/PhysRevResearch.5.033099

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.768_Ni2Mo3O8.mcif from MAGNDATA · entry page

sha256 of this copy: a2402c9068db23241006b2e58782508b33a6e6f4e963a491ba468f2e04844c66
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.768_Ni2Mo3O8.mcif.