Research/Sitter/MAGNDATA / 1.1.115_UPd2Ge2.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of UPd2Ge2Spin lattice of UPd2Ge2

UPd2Ge2

MAGNDATA entry 1.1.115 · 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 ≤ 135 K (−138 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupI4/mmm1′(0,0,γ)00sss
Point group4/mmm1′
Parent space groupI 4/m m m No. 139
Repeats every1.37 cells along c (not a whole number: that's what incommensurate means)
Propagation[0 0 0.7302] 1k
Cella 4.2 · b 4.2 · c 10.23 Å · α 90° · β 90° · γ 90°
Transition135 K (−138 °C)
Measured at100 K
Magnetic ionsU
Largest moment component2.49 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 I4/mmm1′(0,0,γ)00sss →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Pd1Pd00.50.25
U1U000
Ge1Ge000.383

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 (μB), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

G. Andre et al. Solid State Communications (1996) · doi:10.1016/0038-1098(95)00818-7

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.1.115_UPd2Ge2.mcif from MAGNDATA · entry page

sha256 of this copy: 10f24e8da4e16de40b46bf793f5c673ad1f7f97a1120ee6b739189c97ff4da80
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.115_UPd2Ge2.mcif.