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Spin lattice of Fe4O5Spin lattice of Fe4O5

Fe4O5

MAGNDATA entry 0.999 · 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 ≤ 320 K (47 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC m′ c 21′ BNS 36.174
Point groupm′m2′
Parent space groupC m c m No. 63
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 2.8906 · b 9.8024 · c 12.5804 Å · α 90° · β 90° · γ 90°
Transition320 K (47 °C)
Measured at150 K
Magnetic ionsFe
Largest moment component3 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 m′ c 21′ →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe00.50520.2500−33
Fe2Fe0000033
Fe3_1Fe00.26040.11740033
Fe3_2Fe00.26040.38260033
O1_1O00.3590.5442
O1_2O00.3590.9558
O2O00.16010.25
O3_1O00.0930.6422
O3_2O00.0930.8578

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. V. Ovsyannikov et al. Nature Chemistry (2016) · doi:10.1038/nchem.2478

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.999_Fe4O5.mcif from MAGNDATA · entry page

sha256 of this copy: 15983b9a14099a09add5179f4792f4cf471c9598c0df87aa4167ffa6758373a5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.999_Fe4O5.mcif.