Research/Sitter/MAGNDATA / 0.334_CoF3.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of CoF3Spin lattice of CoF3

CoF3

MAGNDATA entry 0.334 · 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 ¹3̄²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 460 K (187 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupR 3 c BNS 167.103
Parent space groupR 3 c No. 167
Spinscollinear · 3 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.03473 · b 5.03473 · c 13.2228 Å · α 90° · β 90° · γ 120°
Transition460 K (187 °C)
Measured at295 K
Magnetic ionsCo
Largest moment component3.21 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 R 3 c →
Atom sites · 2 sites · CSV
siteelementxyzmambmc|m| (μB)
Co1Co000003.213.21
F1F0.604800.25

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

S. Lee et al. Physica B: Physics of Condensed Matter (2018) · doi:10.1016/j.physb.2017.11.082

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.334_CoF3.mcif from MAGNDATA · entry page

sha256 of this copy: c7df2a90d8ab2f443e3f942f3624c20ad8d388616d6637ccd32c218b446d9135
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.334_CoF3.mcif.