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Spin lattice of Na2Ni2TeO6Spin lattice of Na2Ni2TeO6

Na2Ni2TeO6

MAGNDATA entry 1.646 · 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 ≤ 30 K (−243 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupIa m m 2 BNS 44.234
Point groupmm21′
Parent space groupP 63/m c m No. 193
Spinscollinear · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 10.3828 · b 5.19141 · c 22.182 Å · α 90° · β 90° · γ 120°
Transition30 K (−243 °C)
Measured at4 K
Magnetic ionsNi
Largest moment component1.55 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 Ia m m 2 →
Atom sites · 12 sites · CSV
siteelementxyzmambmc|m| (μB)
Te1Te000
Ni1Ni0.16670.66670001.551.55
O1_1O0.163600.2964
O1_2O00.32710.2964
O1_3O0.836500.5464
O1_4O00.67290.5464
Na1_1Na0.174700.125
Na1_2Na00.34950.125
Na1_3Na0.825300.375
Na1_4Na00.65050.375
Na2_1Na0.16670.66670.125
Na2_2Na0.33330.33330.375

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

A. M. Samarakoon et al. Phys. Rev. B (2021) · doi:10.1103/PhysRevB.104.184415

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.646_Na2Ni2TeO6.mcif from MAGNDATA · entry page

sha256 of this copy: 0d030105839dd74840e3899cc53e29fb961e4238653d10e31d88f3635df6a380
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.646_Na2Ni2TeO6.mcif.