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Spin lattice of Tb2Ir3Ga9Spin lattice of Tb2Ir3Ga9

Tb2Ir3Ga9

MAGNDATA entry 0.706 · 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 ²m²m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 12.5 K (−261 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC m′ c m′ BNS 63.464
Parent space groupC m c m No. 63
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 12.986 · b 7.5325 · c 9.4349 Å · α 90° · β 90° · γ 90°
Transition12.5 K (−261 °C)
Measured at10 K
Magnetic ionsIr, Tb
Largest moment component7.5 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 m′ →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb0.3360.33360.257.5007.5
Ir1Ir0.328300
Ir2Ir000
Ga1Ga0.16710.16770.0787
Ga2Ga0.10370.44270.25
Ga3Ga00.33310.5633
Ga4Ga00.12930.25

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. A. Khan et al. PHYSICAL REVIEW MATERIALS (2019) · doi:10.1103/PhysRevMaterials.3.114411

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.706_Tb2Ir3Ga9.mcif from MAGNDATA · entry page

sha256 of this copy: 50fdbcfcc6830f7d5b183342495a6619ae71c27580f4f4047a85b3ce4f951097
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.706_Tb2Ir3Ga9.mcif.