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Spin lattice of Ba2Nd1Ru1O6Spin lattice of Ba2Nd1Ru1O6

Ba2Nd1Ru1O6

MAGNDATA entry 0.1013 · 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 ≤ 58 K (−215 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 1 BNS 2.4
Point group1
Parent space groupP 21/n No. 14
Spinscollinear · 1 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.9715 · b 5.9709 · c 8.4761 Å · α 90° · β 90° · γ 90°
Transition58 K (−215 °C)
Measured at7 K
Magnetic ionsNd, Ru
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 1 →
Atom sites · 12 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1_1Ba0.0190.0010.246
Ba1_2Ba0.4810.5010.254
Nd1_1Nd0.5001.63−1.6302.3052
Nd1_2Nd00.50.5−1.631.6302.3052
Ru1_1Ru0.500.5−1.561.5602.2062
Ru1_2Ru00.501.56−1.5602.2062
O1_1O0.2150.250.007
O1_2O0.2850.750.493
O2_1O0.2160.7490.007
O2_2O0.2840.2490.493
O3_1O0.9730.4860.232
O3_2O0.5270.9860.268

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

Y. Izumiyama et al. J. Mater. Chem. (2000) · doi:10.1039/b003629n

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1013_Ba2NdRuO6.mcif from MAGNDATA · entry page

sha256 of this copy: 51b05d9de8b471ad80020eb333b203e8b956121bce54934371098d6c524cc8f7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1013_Ba2NdRuO6.mcif.