Research/Sitter/MAGNDATA / 1.659_MnCl2(CO(NH2)2)2.mcif

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Spin lattice of MnCl2C2O2N4H8Spin lattice of MnCl2C2O2N4H8

MnCl2C2O2N4H8

MAGNDATA entry 1.659 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 3 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPI c a 21 BNS 29.110
Point groupmm21′
Parent space groupI b a 2 No. 45
Spinscollinear · net moment 0 μB per cell
Propagation[1 1 1] 1k
Cella 9.163 · b 12.5772 · c 7.3398 Å · α 90° · β 90° · γ 90°
Transition2.99 K (−270 °C)
Measured at1.4 K
Magnetic ionsMn
Largest moment component4.06 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 PI c a 21 →
Atom sites · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
MnMn000.314304.0604.06
ClCl0.80030.00860.063
OO0.98280.16790.3236
CC0.07140.24410.3228
N1N0.03620.33570.4021
H1H0.9510.34070.4575
H2H0.09040.39280.4134
N2N0.20020.23660.2414
H3H0.23040.17720.1914
H4H0.26670.28540.2637

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

J. L. Manson et al. Inorg. Chem. (2015) · doi:10.1021/acs.inorgchem.5b02162

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.659_MnCl2(CO(NH2)2)2.mcif from MAGNDATA · entry page

sha256 of this copy: d934e206e79a760b94a9919eeee718d5f8e7d760b2112a49ff8fbae7bb893ff5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.659_MnCl2(CO(NH2)2)2.mcif.