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Spin lattice of TmMn3O6Spin lattice of TmMn3O6

TmMn3O6

MAGNDATA entry 0.231 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 28 K (−245 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP m m′ n′ BNS 59.410
Parent space groupP m m n No. 59
Spinscollinear · net moment 2.726 μB per cell
Propagation[0 0 0] 1k
Cella 7.2294 · b 7.4108 · c 7.7258 Å · α 90° · β 90° · γ 90°
Transition28 K (−245 °C)
Measured at1.5 K
Magnetic ionsMn, Tm
Largest moment component3.7 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 m m′ n′ →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Tm1Tm0.250.250.78440−0.7700.77
Tm2Tm0.250.250.28590−3.703.7
Mn1Mn0.250.750.277302.00302.003
Mn2Mn0.250.750.76250−3.1703.17
Mn3Mn00001.9101.91
Mn4Mn000.501.5901.59
O1O0.4355−0.06810.2671
O2O0.05820.250.0451
O3O0.250.52810.9202
O4O0.54030.250.4177
O5O0.250.43070.5408

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. Vibhakar et al. Physical Review B (2019) · doi:10.1103/PhysRevB.99.104424

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.231_TmMn3O6.mcif from MAGNDATA · entry page

sha256 of this copy: 3ae3e55bf9c8dd96482ba9c5bdb36392f63d3c82f1c65174fe4a7cf803cb5a71
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.231_TmMn3O6.mcif.