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Spin lattice of Ba(TiO)Cu4(PO4)4Spin lattice of Ba(TiO)Cu4(PO4)4

Ba(TiO)Cu4(PO4)4

MAGNDATA entry 1.235 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 9.5 K (−264 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPc 42 21 2 BNS 94.132
Parent space groupP 4 21 2 No. 90
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 9.6028 · b 9.6028 · c 14.2418 Å · α 90° · β 90° · γ 90°
Transition9.5 K (−264 °C)
Measured at1.5 K
Magnetic ionsCu
Largest moment component0.57 μB
MethodNPD and single crystal neutron polarimetry (SNP)

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 Pc 42 21 2 →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba000
Cu1Cu0.2680.98810.20210.560.03−0.570.7996
Ti1Ti00.50.0102
P1P0.28150.19210.3699
O1O0.34930.13510.2783
O2O0.12470.16210.3659
O3O0.33740.11160.4548
O4O00.50.3915
O5O0.31730.34730.3765

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

P. Babkevich et al. Phys. Rev. B (2017) · doi:10.1103/PhysRevB.96.214436

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.235_Ba(TiO)Cu4(PO4)4.mcif from MAGNDATA · entry page

sha256 of this copy: 72324eb087ee50bef3fb947fbf4d29a42fff22449980b6f3f983d64033fcbac0
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.235_Ba(TiO)Cu4(PO4)4.mcif.