Research/Sitter/MAGNDATA / 1.787_RuCl3.mcif

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Spin lattice of Ru1Cl3Spin lattice of Ru1Cl3

Ru1Cl3

MAGNDATA entry 1.787 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹1̄ × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 6.3 K (−267 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPS 1 BNS 2.7
Point group11′
Parent space groupR 3 No. 148
Spinscollinear · net moment 0 μB per cell
Propagation[0 1/2 1] 1k
Cella 5.973 · b 11.946 · c 16.93 Å · α 90° · β 90° · γ 120°
Transition6.3 K (−267 °C)
Measured at4 K
Magnetic ionsRu
Largest moment component0.54 μB
MethodNeutron single crystal data

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 PS 1 →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Ru1Ru000.3330.4900.540.7292
Cl1_1Cl0.31780.1670.4118
Cl1_2Cl0.6660.99190.4118
Cl1_3Cl0.01620.84110.4118

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

S.-Y. Park et al. J. Phys.: Condens. Matter (2024) · doi:10.1088/1361-648X/ad294f

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.787_RuCl3.mcif from MAGNDATA · entry page

sha256 of this copy: 953bb54b4235f95c8436a9eabedc1716d420f1b90545dd4dd039d641ec7dbe1c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.787_RuCl3.mcif.