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Spin lattice of Ba6Co6ClO15.5Spin lattice of Ba6Co6ClO15.5

Ba6Co6ClO15.5

MAGNDATA entry 1.275 · 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 ¹6/¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 135 K (−138 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 9 properties
Magnetic groupPc 6 c 2 BNS 188.220
Parent space groupP 6 m 2 No. 187
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 5.671 · b 5.671 · c 28.912 Å · α 90° · β 90° · γ 120°
Transition135 K (−138 °C)
Magnetic ionsCo
Largest moment component2.85 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 Pc 6 c 2 →
Atom sites · 12 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba000.1016
Ba2Ba0.66670.33330.1769
Ba3Ba000.25
Ba4Ba0.33330.66670
Co1Co0.33330.66670.1227000.530.53
Co2Co0.33330.66670.2084000.540.54
Co3Co0.66670.33330.0607002.852.85
Cl1Cl000
O1O0.49160.50840.0834
O2O0.18560.81440.1666
O3O0.48240.51760.25
O4O0.71080.28920

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. Mentre et al. Solid State Sciences (2008) · doi:10.1016/j.solidstatesciences.2007.12.032

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.275_Ba6Co6ClO15.5.mcif from MAGNDATA · entry page

sha256 of this copy: 6165f024ee854015fa5620de322a89864b11c1037526a64821f18851513b54cd
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.275_Ba6Co6ClO15.5.mcif.