Research/Sitter/MAGNDATA / 0.1153_Bi2NiO2F4.mcif

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Spin lattice of Bi2Ni1O2F4Spin lattice of Bi2Ni1O2F4

Bi2Ni1O2F4

MAGNDATA entry 0.1153 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 45 K (−228 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP c a 21 BNS 29.99
Point groupmm2
Parent space groupP 21 a b No. 29
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.414 · b 5.4137 · c 16.0399 Å · α 90° · β 90° · γ 90°
Transition45 K (−228 °C)
Measured at1.5 K
Magnetic ionsNi
Largest moment component1.1 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 c a 21 →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Bi1Bi0.0310.50.5803
Bi2Bi0.0370.0060.0796
Ni1Ni0.040.5050.24271.100.71.3038
F1F0.2510.2120.284
F2F0.9720.4860.1302
F3F0.9890.5240.3731
F4F0.3450.6950.2497
O1O0.2820.2470.999
O2O0.2780.7530.5082

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

Olivier Mentre et al. Chem. Mater. (2022) · doi:10.1021/acs.chemmater.2c01213

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1153_Bi2NiO2F4.mcif from MAGNDATA · entry page

sha256 of this copy: 021c35c5b3a551cc6239da5ed8d03203ec646d30f6e0c32f56ca1adfe0a52a42
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1153_Bi2NiO2F4.mcif.