Research/Sitter/MAGNDATA / 1.840_Sr2Mn2O5.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Sr2Mn2O5Spin lattice of Sr2Mn2O5

Sr2Mn2O5

MAGNDATA entry 1.840 · 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 ≤ 390 K (117 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPc b a m BNS 55.361
Point groupmmm1′
Parent space groupP b a m No. 55
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 5.51045 · b 10.75403 · c 7.61716 Å · α 90° · β 90° · γ 90°
Transition390 K (117 °C)
Measured at4.2 K
Magnetic ionsMn
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 Pc b a m →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
SrSr0.28850.36390.25
MnMn0.26120.120400.533.4403.4806
O1O0.28830.10370.25
O2O0.53070.22670
O3O000

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

V. Caignaert et al. J. Magn. Magn. Mater. (1997) · doi:10.1016/S0304-8853(96)00455-6

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.840_Sr2Mn2O5.mcif from MAGNDATA · entry page

sha256 of this copy: 8e08f79b6db3973a2c34b69e87a50954da2f49192e1804be178ff5b9c88e59b1
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.840_Sr2Mn2O5.mcif.