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Spin lattice of TmMn3O6Spin lattice of TmMn3O6

TmMn3O6

MAGNDATA entry 0.232 · 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 ≤ 74 K (−199 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP m′ m′ n BNS 59.409
Parent space groupP m m n No. 59
Spinscollinear · net moment 11.594 μB per cell
Propagation[0 0 0] 1k
Cella 7.2294 · b 7.4108 · c 7.7258 Å · α 90° · β 90° · γ 90°
Transition74 K (−199 °C)
Measured at40 K
Magnetic ionsMn, Tm
Largest moment component3.1 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)
Tm1Tm0.250.250.7844
Tm2Tm0.250.250.2859
Mn1Mn0.250.750.2773001.9571.957
Mn2Mn0.250.750.762500−3.13.1
Mn3Mn000001.891.89
Mn4Mn000.5001.581.58
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

⬇ 0.232_TmMn3O6.mcif from MAGNDATA · entry page

sha256 of this copy: d4571054221394403de0be4ce4d4dfff062b26b6f5aa3e541d64d11e90b3fe1e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.232_TmMn3O6.mcif.