Research/Sitter/MAGNDATA / 1.801_Tb3NbO7.mcif

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Spin lattice of Tb3Nb1O7Spin lattice of Tb3Nb1O7

Tb3Nb1O7

MAGNDATA entry 1.801 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 2 K (−271 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPB 21 21 2 BNS 18.22
Point group2221′
Parent space groupC 2 2 21 No. 20
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[1 0 0] 1k
Cella 7.469 · b 7.5057 · c 10.5564 Å · α 90° · β 90° · γ 90°
Transition2 K (−271 °C)
Measured at1.8 K
Magnetic ionsTb
Largest moment component7.22 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 PB 21 21 2 →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb0.48820.250.7507.221.167.3126
Tb2Tb0.26790.0050.48463.661.576.487.606
Nb1Nb−0.00930.250.75
O1O0.2070.77150.6287
O2O0.18550.21370.6245
O3O000.3784
O4O000.1148
O5O000.8176

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. Hase et al. Journal of Magnetism and Magnetic Materials (2024) · doi:10.1016/j.jmmm.2024.172106

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.801_Tb3NbO7.mcif from MAGNDATA · entry page

sha256 of this copy: 01a2e9124ef62aae5818af866328a8ec60b0f7973d2e6d8168f6b6b8f0cb2499
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.801_Tb3NbO7.mcif.