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Spin lattice of La0.75Bi0.25Fe0.5Cr0.5O3Spin lattice of La0.75Bi0.25Fe0.5Cr0.5O3

La0.75Bi0.25Fe0.5Cr0.5O3

MAGNDATA entry 0.373 · 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 ¹m²m²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 350 K (77 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n m a BNS 62.441
Parent space groupP n m a No. 62
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.5164 · b 7.7907 · c 5.5209 Å · α 90° · β 90° · γ 90°
Transition350 K (77 °C)
Measured at4 K
Magnetic ionsFe
Largest moment component3.3 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 n m a →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
La1La0.97330.250.0069
Bi1Bi0.97330.250.0069
Fe1Fe000.53.3003.3
Cr1Cr000.5
O1O0.51330.250.918
O2O0.71590.0350.2803

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. Ivanov et al. Journal of Solid State Chemistry (2017) · doi:10.1016/j.jssc.2017.06.031

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.373_La0.75Bi0.25Fe0.5Cr0.5O3.mcif from MAGNDATA · entry page

sha256 of this copy: 275bdd03fcd216ee1367f17261c07dd2950c1c596f3bc975892b2eb7442e860f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.373_La0.75Bi0.25Fe0.5Cr0.5O3.mcif.