Research/Sitter/MAGNDATA / 1.0.24_ThMn2.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of ThMn2Spin lattice of ThMn2

ThMn2

MAGNDATA entry 1.0.24 · 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 ≤ 115 K (−158 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 6′2′m BNS 189.223
Parent space groupP 63/m m c No. 194
Spinscoplanar · net moment 0 μB per cell
Propagation[1/3 1/3 0] 1k
Cella 16.455 · b 16.455 · c 8.896 Å · α 90° · β 90° · γ 120°
Transition115 K (−158 °C)
Measured at5 K
Magnetic ionsMn, Th
Largest moment component1.6 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 P 6′2′m →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Th1_1Th0.11110.22220.062
Th1_2Th0.22220.11110.562
Th1_3Th0.22220.44440.562
Mn1Mn000
Mn2_1Mn0.27770.55530.25−1.6001.6
Mn2_2Mn0.44470.72230.25−1.6001.6
Mn2_3Mn0.72230.44470.751.6001.6
Mn2_4Mn0.55530.27770.751.6001.6

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. Deportes et al. Journal of Magnetism and Magnetic Materials (1987) · doi:10.1016/0304-8853(87)90402-1

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.0.24_ThMn2.mcif from MAGNDATA · entry page

sha256 of this copy: 589e4eac5fef90ab106de622b11c9fd43eaa62c9d336b94ec13e6119a43ba273
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.24_ThMn2.mcif.