Research/Sitter/MAGNDATA / 0.582_Fe3F8(H2O)2.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Fe3F8(H2O)2Spin lattice of Fe3F8(H2O)2

Fe3F8(H2O)2

MAGNDATA entry 0.582 · 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 ²2/²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 157 K (−116 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2′/m′ BNS 12.62
Parent space groupC 2/m No. 12
Spinscollinear · 1 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 7.544 · b 7.4324 · c 7.387 Å · α 90° · β 117.26° · γ 90°
Transition157 K (−116 °C)
Measured at40 K
Magnetic ionsFe
Largest moment component3.98 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 C 2′/m′ →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe0.250.250.503.9803.98
Fe2Fe00.50
F1F00.29920.5
F2F0.178100.4394
F3F0.13360.29620.2126
O1O0.24700.0555
H1H0.2090.10020.108

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

M. Leblanc et al. Journal of Magnetism and Magnetic Materials (1991) · doi:10.1016/0304-8853(91)90849-6

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.582_Fe3F8(H2O)2.mcif from MAGNDATA · entry page

sha256 of this copy: a42bad2228568a066c38e0f48d979e6bfa3b63665fa1ec421b8046bc9dc02ad5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.582_Fe3F8(H2O)2.mcif.