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Spin lattice of Cs2FeCl5.D2OSpin lattice of Cs2FeCl5.D2O

Cs2FeCl5.D2O

MAGNDATA entry 0.252 · 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 ¹2/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 6.6 K (−267 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2′/c BNS 15.87
Parent space groupC 2/c No. 15
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 17.051 · b 7.3527 · c 16.1364 Å · α 90° · β 89.95° · γ 90°
Transition6.6 K (−267 °C)
Measured at1.8 K
Magnetic ionsFe
Largest moment component4.39 μB
MethodNSD and NPD

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′/c →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe0.87810.00410.62520−4.3904.39
Cl1Cl0.74410.00640.6226
Cl2Cl0.89140.78990.514
Cl3Cl0.88780.2430.5289
Cl4Cl0.89130.21910.7363
Cl5Cl0.88360.76830.7243
O1O0.00590.99240.6264
Cs1Cs0.97090.52440.8748
Cs2Cs0.7430.49240.1247
D1D0.03180.04230.5767
D2D0.03330.04520.6728

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

O. Fabelo et al. PHYSICAL REVIEW B (2017) · doi:10.1103/PhysRevB.96.104428

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.252_Cs2FeCl5.D2O.mcif from MAGNDATA · entry page

sha256 of this copy: 567b76facba77a9365393610af7f5f77f10fa575cea1a99cad8094a1eafab589
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.252_Cs2FeCl5.D2O.mcif.