Research/Sitter/MAGNDATA / 0.307_ScCrO3.mcif

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Spin lattice of ScCrO3Spin lattice of ScCrO3

ScCrO3

MAGNDATA entry 0.307 · 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 ≤ 73 K (−200 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n m a BNS 62.441
Point groupmmm
Parent space groupP n m a No. 62
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.3613 · b 7.3847 · c 5.0296 Å · α 90° · β 90° · γ 90°
Transition73 K (−200 °C)
Measured at1.5 K
Magnetic ionsCr
Largest moment component2.7 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 · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Sc1Sc0.07090.25−0.0211
Cr1Cr000.502.702.7
O1O0.44180.250.1294
O2O0.30720.06940.6887

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

L. Ding et al. PHYSICAL REVIEW B (2017) · doi:10.1103/PhysRevB.95.054432

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.307_ScCrO3.mcif from MAGNDATA · entry page

sha256 of this copy: 06afd9a8659dcf6c2ac1bf5d65812e0cc5fdcca9ab67f932acd0e9592760a0a5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.307_ScCrO3.mcif.