Research/Sitter/MAGNDATA / 1.657_LuNiO3.mcif

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Spin lattice of LuNiO3Spin lattice of LuNiO3

LuNiO3

MAGNDATA entry 1.657 · 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 ≤ 125 K (−148 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPa 21 BNS 4.10
Point group21′
Parent space groupP 21/n No. 14
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 10.2087 · b 5.4972 · c 14.6504 Å · α 90° · β 90.18° · γ 90°
Transition125 K (−148 °C)
Measured at2 K
Magnetic ionsNi
Largest moment component1.03 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 Pa 21 →
Atom sites · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
Ni1Ni0.2500101.031.4333
Ni2Ni0.2500.250.480−0.490.687
Lu1_1Lu0.48990.07910.1257
Lu1_2Lu0.51010.92090.8743
O1_1O0.05560.46180.1216
O1_2O0.94450.53820.8783
O2_1O0.34720.30940.026
O2_2O0.65290.69060.974
O3_1O0.09060.20050.4711
O3_2O0.90940.79950.529

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

F. Serrano-Sanchez et al. Dalton Trans. (2021) · doi:10.1039/d1dt03571a

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.657_LuNiO3.mcif from MAGNDATA · entry page

sha256 of this copy: 0dfc3e2637ecbbb42faa941057104e2dd8762e36fe1c929d7e94f6e65f567035
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.657_LuNiO3.mcif.