Research/Sitter/MAGNDATA / 0.528_CrSb.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of CrSbSpin lattice of CrSb

CrSb

MAGNDATA entry 0.528 · source
g-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. g-wave: 4 nodal planes.
Spin group ²6/²m¹m²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered > 600 K (327 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 63′/m′ m′ c BNS 194.268
Parent space groupP 63/m m c No. 194
Spinscollinear · 4 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 4.103 · b 4.103 · c 5.463 Å · α 90° · β 90° · γ 120°
Transition>600 K (327 °C)
Measured at295 K
Magnetic ionsCr
Largest moment component2.45 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 63′/m′ m′ c →
Atom sites · 2 sites · CSV
siteelementxyzmambmc|m| (μB)
Cr1Cr000002.452.45
Sb1Sb0.33330.66670.25

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. Yuan et al. Dalton Trans. (2020) · doi:10.1039/d0dt03277h

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.528_CrSb.mcif from MAGNDATA · entry page

sha256 of this copy: 40a7843210cf3adc26b1b68b1b37f6973770feb1db7d5f45104f3949088f2046
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.528_CrSb.mcif.