Research/Sitter/MAGNDATA / 0.522_La2O3FeMnSe2.mcif

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Spin lattice of La2O3FeMnSe2Spin lattice of La2O3FeMnSe2

La2O3FeMnSe2

MAGNDATA entry 0.522 · source
d-wave altermagnet
No net magnetisation, yet the electron bands are spin-split: the up and down spin sublattices are related only by a rotation or mirror, never by a shift or inversion. d-wave: the splitting changes sign twice around the Fermi surface (2 nodal planes).
Spin group ²4/¹m¹m²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 76 K (−197 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupI m′ m′ m BNS 71.536
Parent space groupI 4/m m m No. 139
Spinscollinear · 2 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 4.0856 · b 4.0856 · c 18.685 Å · α 90° · β 90° · γ 90°
Transition76 K (−197 °C)
Measured at2 K
Magnetic ionsFe, Mn
Largest moment component3.44 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 I m′ m′ m →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
La1La000.6831
Fe1_1Fe00.503.44003.44
Fe1_2Fe0.500−3.44003.44
Mn1_1Mn00.503.44003.44
Mn1_2Mn0.500−3.44003.44
O1O00.50.25
O2O000.5
Se1Se000.0995

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

S. Landsgesell et al. J. Phys.: Condens. Matter (2013) · doi:10.1088/0953-8984/25/8/086004

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.522_La2O3FeMnSe2.mcif from MAGNDATA · entry page

sha256 of this copy: 63a4ac4ebe852cd017202a5684ab71409094d0106456691bd5fbfd1f79dfc524
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.522_La2O3FeMnSe2.mcif.