Research/Sitter/MAGNDATA / 1.15_Er2BaNiO5.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Er2BaNiO5Spin lattice of Er2BaNiO5

Er2BaNiO5

MAGNDATA entry 1.15 · 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 ≤ 33 K (−240 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupCc 2/c BNS 15.90
Point group2/m1′
Parent space groupI m m m No. 71
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 7.5091 · b 5.7319 · c 22.543 Å · α 90° · β 90° · γ 90°
Transition33 K (−240 °C)
Measured at1.5 K
Magnetic ionsHo, Ni
Largest moment component7.89 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 Cc 2/c →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Er1Ho0.2500.10147.8900.257.894
Ba1Ba0.250.50
Ni1Ni000−1.40−0.641.5394
O1O00.24140.0741
O2O0.2500

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

E. Garcia-Matres et al. Solid State Communications (1993) · doi:10.1016/0038-1098(93)90306-8

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.15_Er2BaNiO5.mcif from MAGNDATA · entry page

sha256 of this copy: ba12b6cb8c8995293ae0a54a3862462430104c339b62094e1105b5d491bc35b7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.15_Er2BaNiO5.mcif.