Research/Sitter/MAGNDATA / 0.1083_RuP3SiO11.mcif

Ru₁P₃Si₁O₁₁

MAGNDATA entry 0.1083 · 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 ¹3̄¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.

ordered ≤ 1.3 K (−272 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	R 3′ c′ BNS 167.106
Point group	3′m′
Parent space group	R 3 c No. 167
Spins	collinear · net moment 0 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 8.2297 · b 8.2297 · c 39.2 Å · α 90° · β 90° · γ 120°
Transition	1.3 K (−272 °C)
Measured at	0.08 K
Magnetic ions	Ru
Largest moment component	0.35 μ_B
Method	NPD

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′ c′ →

Atom sites · 8 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Ru1	Ru	0	0	0.1583	0	0	0.35	0.35
P1	P	0.372	0.0381	0.1196
Si1	Si	0	0	0.0397
O1	O	0.0484	0.2042	0.0533
O2	O	0.2273	0.0877	0.1273
O3	O	0.1377	0.2316	0.1891
O4	O	0.792	0	0.25
O5	O	0	0	0

Moment components are along the crystal axes a, b, c (μ_B), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

Aly. H. Abdeldaim et al. Nature Communications (2024) · doi:10.1038/s41467-024-53900-3

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1083_RuP3SiO11.mcif from MAGNDATA · entry page

sha256 of this copy: bbbe109aaffb0c34ca444ac3eb8caf33da2dff4540456dfd803e89dc027e8cc1
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1083_RuP3SiO11.mcif.

Ru1P3Si1O11

Symmetry

Source

Original file

Ru₁P₃Si₁O₁₁