Research/Sitter/MAGNDATA / 0.944_Yb2Ir2O7.mcif

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Spin lattice of Yb2Ir2O7Spin lattice of Yb2Ir2O7

Yb2Ir2O7

MAGNDATA entry 0.944 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 2 K (−271 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupR 3 m′ BNS 166.101
Point group3m′
Parent space groupF d 3 m No. 227
Spinsnoncoplanar · net moment 9.145 μB per cell
Propagation[0 0 0] 1k
Cella 10.104 · b 10.104 · c 10.104 Å · α 90° · β 90° · γ 90°
Transition2 K (−271 °C)
Measured at0.04 K
Magnetic ionsIr, Yb
Largest moment component0.33 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 R 3 m′ →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Yb1_1Yb0.50.50.50.330.330.330.5716
Yb1_2Yb0.250.7500.330.330.330.5716
Ir1_1Ir0000.2540.2540.2540.4399
Ir1_2Ir0.750.250.5−0.254−0.2540.2540.4399
O1O0.3750.3750.375
O2_1O0.340.1250.125
O2_2O0.410.1250.625

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

H. Jacobsen et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.101.104404

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.944_Yb2Ir2O7.mcif from MAGNDATA · entry page

sha256 of this copy: 9809d23db53b6a07e7b6ebd593673a6ff8c18cbf3ae926ac9ebad457efe83263
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.944_Yb2Ir2O7.mcif.