Research/Sitter/MAGNDATA / 0.271_Tb2MnNiO6.mcif

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Spin lattice of Tb2MnNiO6Spin lattice of Tb2MnNiO6

Tb2MnNiO6

MAGNDATA entry 0.271 · source
s-wave ferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Spin group ¹2/¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 120 K (−153 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21′/c′ BNS 14.79
Parent space groupP 21/c No. 14
Spinscollinear · net moment 6.767 μB per cell
Propagation[0 0 0] 1k
Cella 5.2728 · b 5.5181 · c 7.5104 Å · α 90° · β 90.165° · γ 90°
Transition120 K (−153 °C)
Measured at75 K
Magnetic ionsMn, Ni, Tb
Largest moment component1.85 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 P 21′/c′ →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb0.0170.0660.749
Ni1Ni0.500.50.5601.231.35
Mn1Mn0.5000.8501.852.0337

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

J.L. Garcia-Munoz et al. Phys. Rev. B (2019) · doi:10.1103/PhysRevB.99.184444

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.271_Tb2MnNiO6.mcif from MAGNDATA · entry page

sha256 of this copy: 9043668f999ab19d1dbf7150054c6aa7da5fc7e25b3e698f40e869b1a6f89e39
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.271_Tb2MnNiO6.mcif.