Research/Sitter/MAGNDATA / 2.46_Pb2BaCuFeO5Cl.mcif

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Spin lattice of Pb2BaCuFeO5ClSpin lattice of Pb2BaCuFeO5Cl

Pb2BaCuFeO5Cl

MAGNDATA entry 2.46 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Structure · 9 properties
Magnetic groupPC 2 BNS 3.6
Parent space groupP 4/m m m No. 123
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 1/2 1/2] · [1/2 1/2 0] 2k
Cella 5.5504 · b 5.5504 · c 22.5082 Å · α 90° · β 90° · γ 90°
Measured at5 K
Magnetic ionsFe
Largest moment component2.3 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 PC 2 →
Atom sites · 15 sites · CSV
siteelementxyzmambmc|m| (μB)
Pb1_1Pb00.50.0821
Pb1_2Pb00.50.5821
Ba1Ba00.50.25
Cu1_1Cu000.1598
Cu1_2Cu000.6598
Fe1_1Fe000.159802.30.822.4418
Fe1_2Fe000.65980−1.2−0.821.4534
O1_1O000.2542
O1_2O000.7542
O2_1O0.750.250.1451
O2_2O0.250.250.1451
O2_3O0.750.250.6451
O2_4O0.250.250.6451
Cl1_1Cl000
Cl1_2Cl000.5

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

R.K. Li et al. PHYSICAL REVIEW B (2002) · doi:10.1103/PhysRevB.65.104439

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.46_Pb2BaCuFeO5Cl.mcif from MAGNDATA · entry page

sha256 of this copy: e84df060e6cc643a0df8f93132c180914dfd4d16ef1069fe862e1d95763b8ed6
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.46_Pb2BaCuFeO5Cl.mcif.