Research/Sitter/MAGNDATA / 0.132_Fe(N(CN2))2.mcif

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Spin lattice of Fe(N(CN2))2Spin lattice of Fe(N(CN2))2

Fe(N(CN2))2

MAGNDATA entry 0.132 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 19 K (−254 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n n′ m′ BNS 58.398
Point groupm′m′m
Parent space groupP n n m No. 58
Spinscoplanar · net moment 2.02 μB per cell
Propagation[0 0 0] 1k
Cella 6.0362 · b 7.1195 · c 7.4455 Å · α 90° · β 90° · γ 90°
Transition19 K (−254 °C)
Measured at1.7 K
Magnetic ionsFe
Largest moment component3.99 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 n n′ m′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe000−3.991.0104.1158
C1C0.2724−0.14540.3493
N1N0.2165−0.09330.2085
N2N0.15730.27930

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. Lappas et al. Physical Review B (2003) · doi:10.1103/PhysRevB.67.144406

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.132_Fe(N(CN2))2.mcif from MAGNDATA · entry page

sha256 of this copy: 51b4b449716ab29d042086aaa0511e7dfeac558b1ea88e531449bd0537e105ee
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.132_Fe(N(CN2))2.mcif.