Research/Sitter/MAGNDATA / 1.1.7_TbMnO3.mcif

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Spin lattice of TbMnO3Spin lattice of TbMnO3

TbMnO3

MAGNDATA entry 1.1.7 · source
incommensurate spiral
Incommensurate: the magnetic pattern repeats every so many cells, but not a whole number of them, so it never lines up with the crystal lattice. Here it's a spiral: the spin direction rotates as you move along.
ordered ≤ 41 K (−232 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPbn211′(0β0)s00s
Point groupmm21′
Parent space groupP b n m No. 62
Repeats every3.7 cells along b (not a whole number: that's what incommensurate means)
Propagation[0 0.27 0] 1k
Cella 5.297 · b 5.831 · c 7.403 Å · α 90° · β 90° · γ 90°
Transition41 K (−232 °C)
Measured at35 K
Magnetic ionsMn, Tb
Largest moment component3.9 μB
MethodNSD

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 Pbn211′(0β0)s00s →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb−0.0280.0720.25
Mn1Mn0.500
O1O0.0970.460.25
O2O−0.2960.3370.056

Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.

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. Kenzelmann et al. PHYSICAL REVIEW LETTERS (2005) · doi:10.1103/PhysRevLett.95.087206

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.1.7_TbMnO3.mcif from MAGNDATA · entry page

sha256 of this copy: 07fda004e9ad79c7f087c74d84f25b3d05facc3bb8a8a356170f2dc50cee8bc9
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.7_TbMnO3.mcif.