Research/Sitter/MAGNDATA / 2.56_La2O2Fe2OS2.mcif

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Spin lattice of La2O2Fe2OS2Spin lattice of La2O2Fe2OS2

La2O2Fe2OS2

MAGNDATA entry 2.56 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 105 K (−168 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupCa 2/m BNS 12.64
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] · [0 -1/2 1/2] 2k
Cella 8.0706 · b 8.0706 · c 35.6474 Å · α 90° · β 90° · γ 90°
Transition105 K (−168 °C)
Measured at1.8 K
Magnetic ionsFe
Largest moment component3.3 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 Ca 2/m →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
La1_1La000.3402
La1_2La0.250.250.5901
Fe1Fe00.250−3.3003.3
S1_1S000.0467
S1_2S0.250.250.2967
O1_1O00.250.125
O1_2O0.2500.125
O2_1O000.25
O2_2O0.250.250

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. Oogarah et al. Journal of Magnetism and Magnetic Materials (2018) · doi:10.1016/j.jmmm.2017.09.024

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.56_La2O2Fe2OS2.mcif from MAGNDATA · entry page

sha256 of this copy: 97ec0fa8068394693fac30cc06a602a2662c776406222d13416299b534c86e40
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.56_La2O2Fe2OS2.mcif.