Research/Sitter/MAGNDATA / 1.13_Ba3Nb2NiO9.mcif

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Spin lattice of Ba3Nb2Ni1O9Spin lattice of Ba3Nb2Ni1O9

Ba3Nb2Ni1O9

MAGNDATA entry 1.13 · 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 ≤ 4.9 K (−268 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPc 3 1 c BNS 159.64
Point group3m1′
Parent space groupP 3 m 1 No. 164
Spinscoplanar · net moment 0 μB per cell
Propagation[1/3 1/3 3/2] 1k
Cella 17.265 · b 17.265 · c 14.1312 Å · α 90° · β 90° · γ 120°
Transition4.9 K (−268 °C)
Measured at2 K
Magnetic ionsNi
Largest moment component2.08 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 Pc 3 1 c →
Atom sites · 14 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1_1Ba0.11110.22220.8319
Ba1_2Ba0.44440.22220.8319
Ba1_3Ba0.88890.77780.1681
Ba2_1Ba000
Ni1Ni000.251.042.0801.8013
Nb2_1Nb0.11110.22220.0885
Nb2_2Nb0.44440.22220.0885
Nb2_3Nb0.88890.77780.9115
O1_1O0.166700
O1_2O0.83330.66670
O2_1O0.05660.94340.1631
O2_2O0.05660.11320.1631
O2_3O0.11320.05660.8369
O2_4O0.94340.88680.8369

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. Hwang et al. Phys. Rev. Lett. (2012) · doi:10.1103/PhysRevLett.109.257205

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.13_Ba3Nb2NiO9.mcif from MAGNDATA · entry page

sha256 of this copy: 88f00cccba66583cfd4ab124f7dc545c16461bba02cde66ad9b2f40adff6cb8e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.13_Ba3Nb2NiO9.mcif.