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Spin lattice of Ho0.2Bi0.8FeO3Spin lattice of Ho0.2Bi0.8FeO3

Ho0.2Bi0.8FeO3

MAGNDATA entry 0.560 · 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.
Structure · 9 properties
Magnetic groupP n′ m a′ BNS 62.448
Parent space groupP n m a No. 62
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.5436 · b 7.805 · c 5.4042 Å · α 90° · β 90° · γ 90°
Measured at6 K
Magnetic ionsFe
Largest moment component4.7 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 · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Bi1Bi−0.0060.25−0.038
Ho1Ho−0.0060.25−0.038
Fe1Fe000.5004.74.7
O1O0.6280.250.069
O2O0.29490.0292−0.2983

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. Singh et al. AIP Advances (2019) · doi:10.1063/1.5082386

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.560_Ho0.2Bi0.8FeO3.mcif from MAGNDATA · entry page

sha256 of this copy: 91241c87a52ba2baa626b83156c2e6a05dd8c60d48b49cb0bb70835958bc495d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.560_Ho0.2Bi0.8FeO3.mcif.