Research/Sitter/MAGNDATA / 0.151_Tm2Mn2O7.mcif

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Spin lattice of Tm2Mn2O7Spin lattice of Tm2Mn2O7

Tm2Mn2O7

MAGNDATA entry 0.151 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 25 K (−248 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupI 41/a m′ d′ BNS 141.557
Point group4/mm′m′
Parent space groupF d 3m No. 227
Spinsnoncoplanar · net moment 31.76 μB per cell
Propagation[0 0 0] 1k
Cella 6.96471 · b 6.96471 · c 9.84959 Å · α 90° · β 90° · γ 90°
Transition25 K (−248 °C)
Measured at5 K
Magnetic ionsMn, Tm
Largest moment component2.31 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 I 41/a m′ d′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn_1Mn00000.811.661.8471
Tm_1Tm000.50−0.052.312.3105
O1_1O00.250.375
O2_1O00.250.0794
O2_2O0.20440.45440.875

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

E. Pomjakushina et al. Inorg.Chem. (2015) · doi:10.1021/acs.inorgchem.5b01498

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.151_Tm2Mn2O7.mcif from MAGNDATA · entry page

sha256 of this copy: 685f7b2ce2dc7c29ebdb6fc870696211b2fa9d69dcbe113fd3f4b74661ecc7c3
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.151_Tm2Mn2O7.mcif.