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Spin lattice of ErGe1.83Spin lattice of ErGe1.83

ErGe1.83

MAGNDATA entry 0.344 · 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 ≤ 6 K (−267 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC m c 21 BNS 36.172
Parent space groupC m c 21 No. 36
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 4.0523 · b 29.485 · c 3.8846 Å · α 90° · β 90° · γ 90°
Transition6 K (−267 °C)
Measured at1.5 K
Magnetic ionsEr
Largest moment component7.63 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 · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Er1Er00.06090.757.63007.63
Er2Er00.1710.249−7.63007.63
Ge1Ge00.35290.268
Ge2Ge00.40740.744
Ge3Ge00.24990.765
Ge4Ge00.51010.347

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

O. Oleksyn et al. “Journal (1997) · doi:10.1016/S0925-8388(96)02714-4

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.344_ErGe1.83.mcif from MAGNDATA · entry page

sha256 of this copy: 8d327c68ae23566db21728d3011a037d00da5fddeb13898480029838b023497b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.344_ErGe1.83.mcif.