Research/Sitter/MAGNDATA / 1.826_NdZnPO.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Nd1Zn1P1O1Spin lattice of Nd1Zn1P1O1

Nd1Zn1P1O1

MAGNDATA entry 1.826 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹1̄ × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 1.6 K (−272 °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 groupR 3 m No. 166
Spinscollinear · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 7.947 · b 3.9735 · c 61.924 Å · α 90° · β 90° · γ 120°
Transition1.64 K (−272 °C)
Measured at0.3 K
Magnetic ionsNd
Largest moment component1.81 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 · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Nd1Nd000.1906001.811.81
Zn1Zn000.0981
P1P000.0568
O1O000.1526

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

Han Ge et al. PHYSICAL REVIEW B (2024) · doi:10.1103/PhysRevB.110.054443

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.826_NdZnPO.mcif from MAGNDATA · entry page

sha256 of this copy: fdfd598457d8c1bba1474af1938a2d8bd9e5451dd162622078d1ec222cf2f702
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.826_NdZnPO.mcif.