Research/Sitter/MAGNDATA / 1.1.76_Ho2Ni3Si5.mcif

Ho₂Ni₃Si₅

MAGNDATA entry 1.1.76 · source

incommensurate spin-density wave

Incommensurate: the magnetic pattern repeats every so many cells, but not a whole number of them, so it never lines up with the crystal lattice. Here it's a spin-density wave: the size of the spin swells and shrinks as you move along.

ordered ≤ 7.2 K (−266 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	Ibam1′(00γ)0s0s
Point group	mmm1′
Parent space group	I b a m No. 72
Repeats every	3.5 cells along c (not a whole number: that's what incommensurate means)
Propagation	[0 0 0.2855] 1k
Cell	a 9.525 · b 11.059 · c 5.603 Å · α 90° · β 90° · γ 90°
Transition	7.2 K (−266 °C)
Measured at	2 K
Magnetic ions	Ho
Largest moment component	7.9 μ_B
Method	NPD

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 Ibam1′(00γ)0s0s →

Atom sites · 6 sites · CSV

site	element	x	y	z
Ho1	Ho	0.2706	0.374	0
Ni1	Ni	0.1155	0.1382	0
Ni2	Ni	0.5	0	0.25
Si1	Si	0.349	0.126	0
Si2	Si	0	0.26	0.25
Si3	Si	0	0	0.25

Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.

Moment components are along the crystal axes a, b, c (μ_B), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

A. Szytula et al. J. Phys.: Condens. Matter (1997) · doi:10.1088/0953-8984/9/31/017

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.1.76_Ho2Ni3Si5.mcif from MAGNDATA · entry page

sha256 of this copy: 99b6731be3b6c52786486bdbd4aa35871dac049d8a9c0d208b668952712683f6
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.76_Ho2Ni3Si5.mcif.