Research/Sitter/MAGNDATA / 0.415_EuFe2P2.mcif

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Spin lattice of EuFe2P2Spin lattice of EuFe2P2

EuFe2P2

MAGNDATA entry 0.415 · source
s-wave ferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Spin group ¹4/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 30 K (−243 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2′/m′ BNS 12.62
Parent space groupI 4/m m m No. 139
Spinscollinear · net moment 13.197 μB per cell
Propagation[0 0 0] 1k
Cella 3.8165 · b 3.8165 · c 11.166 Å · α 90° · β 90° · γ 90°
Transition30 K (−243 °C)
Measured at3.6 K
Magnetic ionsEu, Fe
Largest moment component6.31 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 C 2′/m′ →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Eu1Eu0001.9306.316.5986
Fe1Fe00.50.25
P1P000.36

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

D.H. Ryan et al. PHYSICAL REVIEW B (2011) · doi:10.1103/PhysRevB.83.132403

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.415_EuFe2P2.mcif from MAGNDATA · entry page

sha256 of this copy: d175170b001d898c195335226896a30342c5fe2faeca6aa809e601196a00492e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.415_EuFe2P2.mcif.