Research/Sitter/MAGNDATA / 0.880_CdCu3(OH)6(NO3)2H2O.mcif

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Spin lattice of CdCu3O13N2H8Spin lattice of CdCu3O13N2H8

CdCu3O13N2H8

MAGNDATA entry 0.880 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 4 K (−269 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC 2/m BNS 12.58
Point group2/m
Parent space groupP 3 m 1 No. 164
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 11.3035 · b 6.5261 · c 6.9989 Å · α 90° · β 90° · γ 90°
Transition4 K (−269 °C)
Measured at1.6 K
Magnetic ionsCu
Largest moment component0.21 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 C 2/m →
Atom sites · 16 sites · CSV
siteelementxyzmambmc|m| (μB)
Cu1_1Cu0.250.250−0.18190.10500.21
Cu1_2Cu00.500−0.2100.21
Cd1Cd000.058
O1_1O0.09110.72680.124
O1_2O0.817900.124
O2O0.666700.782
O3_1O0.1230.6310.511
O3_2O0.75400.511
O4O000.407
N1N0.666700.604
D1_1D0.10080.69760.261
D1_2D0.798400.261
H1_1H0.10080.69760.261
H1_2H0.798400.261
H2_1H0.0350.8950.29
H2_2H0.9300.29

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

Y. Ihara et al. Phys. Rev. B. (2022) · doi:10.1103/PhysRevB.106.024401

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.880_CdCu3(OH)6(NO3)2H2O.mcif from MAGNDATA · entry page

sha256 of this copy: 298d8f09910750bcef6ff5ff2780deda116efd1ab07b5584c714afc760a6a5c9
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.880_CdCu3(OH)6(NO3)2H2O.mcif.