Research/Sitter/MAGNDATA / 0.94_TeNiO3.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of TeNiO3Spin lattice of TeNiO3

TeNiO3

MAGNDATA entry 0.94 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 130 K (−143 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n′ m′ a BNS 62.446
Point groupm′m′m
Parent space groupP n m a No. 62
Spinscoplanar · net moment 3.6 μB per cell
Propagation[0 0 0] 1k
Cella 5.9588 · b 7.5028 · c 5.2143 Å · α 90° · β 90° · γ 90°
Transition130 K (−143 °C)
Measured at2.5 K
Magnetic ionsNi
Largest moment component1.88 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 n′ m′ a →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Te1Te0.98570.250.9815
Ni1Ni000.50−1.880.92.0843
O1O0.0540.250.3424
O2O0.18040.06380.8583

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

M.J. Martinez-Lope et al. Dalton Trans. (2011) · doi:10.1039/c0dt01752c

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.94_TeNiO3.mcif from MAGNDATA · entry page

sha256 of this copy: 29d98f4ce0038504ac5f2976bf2845b18b0d35ba22e17f8500691b72261d1e4e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.94_TeNiO3.mcif.