Research/Sitter/MAGNDATA / 0.234_MnLaMnSbO6.mcif

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Spin lattice of MnLaMnSbO6Spin lattice of MnLaMnSbO6

MnLaMnSbO6

MAGNDATA entry 0.234 · source
s-wave compensated ferrimagnet
Opposite moments cancel, but the two sublattices aren't related by any symmetry, so the bands split like a ferromagnet's (s-wave).
Spin group ¹4/¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 48 K (−225 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 2′/c′ BNS 13.69
Parent space groupP 42/n No. 86
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 7.8634 · b 7.8634 · c 8.0293 Å · α 90° · β 90° · γ 90°
Transition48 K (−225 °C)
Measured at1.5 K
Magnetic ionsMn
Largest moment component4.8 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 2′/c′ →
Atom sites · 14 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn0.250.250.254.8004.8
Mn2Mn0.250.250.754.8004.8
La1_1La0.750.250.2249
La1_2La0.750.250.7249
Mn3_1Mn000−4.8004.8
Mn3_2Mn00.50.5−4.8004.8
Sb1_1Sb000.5
Sb1_2Sb00.50
O1_1O0.9480.5450.228
O1_2O0.4550.4480.728
O2_1O0.7760.9590.578
O2_2O0.0410.2760.078
O3_1O0.7210.080.971
O3_2O0.920.2210.471

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

E. Solana-Madruga et al. Phys. Rev. B (2018) · doi:10.1103/PhysRevB.97.134408

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.234_MnLaMnSbO6.mcif from MAGNDATA · entry page

sha256 of this copy: 53acbe4050a6d4c96a9ccabf4f8e37b17ef9b4fc5c70cb04e5886accdb808d06
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.234_MnLaMnSbO6.mcif.