Research/Sitter/MAGNDATA / 0.912_Ho5Ni2In4.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Ho5Ni2In4Spin lattice of Ho5Ni2In4

Ho5Ni2In4

MAGNDATA entry 0.912 · 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 ≤ 31 K (−242 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21/c BNS 14.75
Point group2/m
Parent space groupP b a m No. 55
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 17.7823 · b 7.8862 · c 3.5735 Å · α 90° · β 90° · γ 90°
Transition31 K (−242 °C)
Measured at25 K
Magnetic ionsHo
Largest moment component5.2 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 21/c →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho000−1.70−5.25.4708
Ho2Ho0.22060.24290
Ho3Ho0.4150.120201.1022.2825
Ni1Ni0.30370.02630.5
In1In0.570.20130.5
In2In0.84890.07130.5

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

C. Ritter et al. J. Phys.: Condens. Matter (2015) · doi:10.1088/0953-8984/27/47/476001

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.912_Ho5Ni2In4.mcif from MAGNDATA · entry page

sha256 of this copy: 7fdc80f550fad1b9acadb0b7a22b2617f2b4e9573a5ccd1934040c16af68a228
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.912_Ho5Ni2In4.mcif.