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Spin lattice of Ba2FeSi2O7Spin lattice of Ba2FeSi2O7

Ba2FeSi2O7

MAGNDATA entry 1.641 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹4/¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 5.2 K (−268 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupCc m c 21 BNS 36.177
Point groupmm21′
Parent space groupP 4 21 m No. 113
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 8.3194 · b 8.3194 · c 10.6672 Å · α 90° · β 90° · γ 90°
Transition5.2 K (−268 °C)
Measured at1.7 K
Magnetic ionsFe
Largest moment component2.085 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 Cc m c 21 →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1_1Ba0.16440.66440.2549
Ba1_2Ba0.66440.83560.7451
Fe1Fe0002.0852.08502.9486
Si1_1Si0.36450.86450.4804
Si1_2Si0.86450.63550.5195
O1_1O00.50.0692
O1_2O0.500.9308
O2_1O0.36510.86510.1321
O2_2O0.86510.63490.8679
O3_1O0.07690.19840.0847
O3_2O0.19840.92310.9153

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

T.-H. Jang et al. PHYSICAL REVIEW B (2021) · doi:10.1103/PhysRevB.104.214434

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.641_Ba2FeSi2O7.mcif from MAGNDATA · entry page

sha256 of this copy: ba46a4769764aa1f9267bda5e38bd40c4295a2927a43a6482e1810197a14efee
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.641_Ba2FeSi2O7.mcif.