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Spin lattice of La2NiO4Spin lattice of La2NiO4

La2NiO4

MAGNDATA entry 0.45 · source
d-wave 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. d-wave: the splitting changes sign twice around the Fermi surface (2 nodal planes).
Spin group ²m¹m²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 80 K (−193 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP c′ c′ n BNS 56.369
Point groupm′m′m
Parent space groupP 42/n c m No. 138
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.4995 · b 5.4995 · c 12.5052 Å · α 90° · β 90° · γ 90°
Transition80 K (−193 °C)
Measured at4 K
Magnetic ionsNi
Largest moment component1.68 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 c′ c′ n →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
La1La−0.0072−0.00720.3639
Ni1Ni0001.68001.68
O1O0.750.750.0155
O2O0.750.250
O3O0.03140.03140.1771

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

J. Rodriguez-Carvajal et al. J. Phys.: Condens. Matter (1991) · doi:10.1088/0953-8984/3/19/002

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.45_La2NiO4.mcif from MAGNDATA · entry page

sha256 of this copy: 8964097790b25ecfd84c9a3e3a7c1635a8d9baacda557a207508d46ccb6f487c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.45_La2NiO4.mcif.