Research/Sitter/MAGNDATA / 0.354_TbCrO3.mcif

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Spin lattice of TbCrO3Spin lattice of TbCrO3

TbCrO3

MAGNDATA entry 0.354 · 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 ²m¹m²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 158 K (−115 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n′ m′ a BNS 62.446
Parent space groupP b n m No. 62
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.291 · b 5.513 · c 7.557 Å · α 90° · β 90° · γ 90°
Transition158 K (−115 °C)
Measured at77 K
Magnetic ionsCr, Tb
Largest moment component2.55 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 · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb0.4890.4360.75
Cr1Cr0.500002.552.55
O1O0.5960.030.75
O2O0.6970.3010.049

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

E.F. Bertaut et al. J. Phys. Chem. Solids (1967) · doi:10.1016/0022-3697(67)90238-7

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.354_TbCrO3.mcif from MAGNDATA · entry page

sha256 of this copy: 32e783a25105e7f561ce041e4d1a970b0392e49883b544c2b309a474eab3cfe0
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.354_TbCrO3.mcif.