Research/Sitter/MAGNDATA / 0.428_BaMn2Si2O7.mcif

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Spin lattice of BaMn2Si2O7Spin lattice of BaMn2Si2O7

BaMn2Si2O7

MAGNDATA entry 0.428 · 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 ¹2/¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 26 K (−247 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2/c BNS 15.85
Parent space groupC 2/c No. 15
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 7.2761 · b 12.9361 · c 14.0012 Å · α 90° · β 90.21° · γ 90°
Transition26 K (−247 °C)
Measured at4 K
Magnetic ionsMn
Largest moment component3.9 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/c →
Atom sites · 13 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba0.20490.47170.126
Mn1Mn00.73740.2503.903.9
Mn2Mn00.2630.2503.903.9
Mn3Mn0.03130.2660.51940−3.903.9
Si1Si0.22920.12690.1301
Si2Si0.32270.40470.3821
O1O0.08770.22170.1105
O2O0.18860.38920.2971
O3O0.2340.1310.5127
O4O0.49080.32440.1381
O5O0.09650.02030.125
O6O0.27670.1480.2449
O7O0.38180.10880.0478

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

J. Ma et al. PHYSICAL REVIEW B (2013) · doi:10.1103/PhysRevB.88.144405

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.428_BaMn2Si2O7.mcif from MAGNDATA · entry page

sha256 of this copy: 48874a3b2a6c4a2ceefc35ab9b8b6e3a5035b97194e9d61919ae03f36d2b3634
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.428_BaMn2Si2O7.mcif.