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Spin lattice of Ho2RhSi3Spin lattice of Ho2RhSi3

Ho2RhSi3

MAGNDATA entry 1.897 · 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 ¹2/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 5.2 K (−268 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPA m c 21 BNS 26.74
Point groupmm21′
Parent space groupP 63/m m c No. 194
Spinscollinear · net moment 0 μB per cell
Propagation[1/2 0 0] 1k
Cella 16.248 · b 8.124 · c 7.761 Å · α 90° · β 90° · γ 120°
Transition5.2 K (−268 °C)
Measured at1.5 K
Magnetic ionsHo
Largest moment component9.18 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 c 21 →
Atom sites · 12 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1_1Ho000.25009.189.18
Ho1_2Ho000.75009.189.18
Ho2_1Ho0.25150.0060.25009.189.18
Ho2_2Ho0.4970.4970.25009.189.18
Ho2_3Ho0.24850.5030.75009.189.18
Ho2_4Ho0.0030.5030.75009.189.18
Rh1_1Rh0.16670.66670.108
Rh1_2Rh0.33330.33330.608
Si1_1Si0.0830.3320.006
Si1_2Si0.4170.1660.506
Si1_3Si0.3340.8340.006
Si1_4Si0.1660.1660.506

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

W. Bazela et al. J. Alloys Compd. (2003) · doi:10.1016/S0925-8388(03)00374-8

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.897_Ho2RhSi3.mcif from MAGNDATA · entry page

sha256 of this copy: 52fef4b76f73b683706ef1698c5cd5c036cb0153b380bf88206280fd1d5dab49
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.897_Ho2RhSi3.mcif.