Research/Sitter/MAGNDATA / 2.103_Eu3PbO.mcif

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Spin lattice of Eu3Pb1O1Spin lattice of Eu3Pb1O1

Eu3Pb1O1

MAGNDATA entry 2.103 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹4/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
Structure · 10 properties
Magnetic groupP m′ m′ m BNS 47.252
Point groupm′m′m
Parent space groupP m 3 m No. 221
Spinscollinear · net moment 10.16 μB per cell
Propagation[1/2 0 0] · [0 0 0] 2k
Cella 10.1564 · b 5.0782 · c 5.0782 Å · α 90° · β 90° · γ 90°
Measured at1.5 K
Magnetic ionsEu
Largest moment component5.08 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 m′ m′ m →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Eu1_1Eu00.50.5005.085.08
Eu1_2Eu0.2500.500−5.085.08
Eu1_3Eu0.250.5000−5.085.08
Eu1_4Eu0.7500.5005.085.08
Eu1_5Eu0.750.50005.085.08
Pb1Pb000
O1_1O0.250.50.5
O1_2O0.750.50.5

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

M. M. Hirschmann et al. PHYSICAL REVIEW MATERIALS (2022) · doi:10.1103/PhysRevMaterials.6.114202

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.103_Eu3PbO.mcif from MAGNDATA · entry page

sha256 of this copy: 3b9d9ab801b8caa2709ca0202a83374ae2d25cabb8a0cab497db0abdbac00c87
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.103_Eu3PbO.mcif.