Research/Sitter/MAGNDATA / 0.669_Sr2YbRuO6.mcif

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Spin lattice of Sr2YbRuO6Spin lattice of Sr2YbRuO6

Sr2YbRuO6

MAGNDATA entry 0.669 · source
altermagnet
No net magnetisation, yet the electron bands are spin-split: the up and down spin sublattices are related only by a rotation or mirror, never by a shift or inversion.
Spin group ²2/²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 36 K (−237 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21/c BNS 14.75
Parent space groupP1121/n No. 14
Spinscollinear · 1 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.7305 · b 8.1021 · c 5.736 Å · α 90° · β 90° · γ 90.2°
Transition36 K (−237 °C)
Measured at2 K
Magnetic ionsRu, Yb
Largest moment component1.63 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 P 21/c →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Sr1Sr0.00550.2480.0258
Yb1Yb0.5000.340.4200.5394
Ru1Ru000.51.321.6302.0939
O1O0.26890.03450.2961
O2O0.20180.03350.7706
O3O0.93630.23780.4876

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. Sharma et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.102.134412

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.669_Sr2YbRuO6.mcif from MAGNDATA · entry page

sha256 of this copy: 616ee265b02f7a23ba9bc52c4b2b85c8b50f6cd2b6895b5cd8dab47d7740a533
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.669_Sr2YbRuO6.mcif.