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Spin lattice of HoC2Spin lattice of HoC2

HoC2

MAGNDATA entry 1.534 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 26 K (−247 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPa m m a BNS 51.298
Parent space groupI 4/m m m No. 139
Spinscollinear · net moment 0 μB per cell
Propagation[3/4 0 0] 1k
Cella 14.532 · b 3.633 · c 6.132 Å · α 90° · β 90° · γ 90°
Transition26 K (−247 °C)
Measured at5 K
Magnetic ionsHo
Largest moment component9.75 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 Pa m m a →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1_1Ho000009.759.75
Ho1_2Ho0.1250.50.500−6.896.89
Ho1_3Ho0.2500
C1_1C000.3957
C1_2C0.1250.50.8957
C1_3C0.2500.3957

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. Atoji et al. J. Chem. Phys. (1967) · doi:10.1063/1.1840950

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.534_HoC2.mcif from MAGNDATA · entry page

sha256 of this copy: 97f82e84708e9a9790b9ee56b252b70c4f5f56ee0558043c783493c28aef95ac
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.534_HoC2.mcif.