Research/Sitter/MAGNDATA / 1.48_HoNiO3.mcif

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Spin lattice of HoNiO3Spin lattice of HoNiO3

HoNiO3

MAGNDATA entry 1.48 · 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 ≤ 145 K (−128 °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 10.364 · b 5.5105 · c 14.8467 Å · α 90° · β 90.084° · γ 90°
Transition145 K (−128 °C)
Measured at10 K
Magnetic ionsHo, Ni
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 Pa 21 →
Atom sites · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1_1Ho−0.00910.07180.1252
Ho1_2Ho0.0091−0.0718−0.1252
Ni1Ni0.25000.901.11.4202
Ni2Ni0.2500.250.350−0.40.5319
O1_1O0.0491−0.530.1224
O1_2O−0.0491−0.47−0.1224
O2_1O0.85−0.690.0247
O2_2O0.15−0.31−0.0247
O3_1O0.0935−0.794−0.0259
O3_2O−0.0935−0.2060.0259

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

M.T. Fernandez-Diaz et al. PHYSICAL REVIEW B (2001) · doi:10.1103/physrevb.64.144417

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.48_HoNiO3.mcif from MAGNDATA · entry page

sha256 of this copy: 5ea3cf20556d5bc7d870f8bfe1642e818d4b9862d5512d29b24fd392d6ba6106
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.48_HoNiO3.mcif.