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Spin lattice of BaCrF5Spin lattice of BaCrF5

BaCrF5

MAGNDATA entry 0.303 · 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 ≤ 3.4 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21′ 21′ 21 BNS 19.27
Parent space groupP 21 21 21 No. 19
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 13.938 · b 5.711 · c 4.947 Å · α 90° · β 90° · γ 90°
Transition3.4 K (−270 °C)
Measured at2.2 K
Magnetic ionsCr
Largest moment component1 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 21′ 21′ 21 →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba0.09230.08990.0178
F1F0.26670.14390.7809
F2F0.42110.18540.0871
F3F0.09180.34810.5564
F4F0.08070.5990.129
F5F0.24790.38730.2326
Cr1Cr0.1650.60260.42470011

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

H. Holler et al. Z. fur Naturforschung B (1982)

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.303_BaCrF5.mcif from MAGNDATA · entry page

sha256 of this copy: e8ab3a42bb802b37840f9228d5a25648e904340af2f4f2ca143b2be0332808ed
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.303_BaCrF5.mcif.