Channel structure in the new BiCoPO5. Comparison with BiNiPO5. Crystal structure, lone pair localisation and infrared characterisation

Citation
M. Ketatni et al., Channel structure in the new BiCoPO5. Comparison with BiNiPO5. Crystal structure, lone pair localisation and infrared characterisation, SOLID ST SC, 1(6), 1999, pp. 449-460
Citations number
21
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
SOLID STATE SCIENCES
ISSN journal
12932558 → ACNP
Volume
1
Issue
6
Year of publication
1999
Pages
449 - 460
Database
ISI
SICI code
1293-2558(199908/09)1:6<449:CSITNB>2.0.ZU;2-U
Abstract
The new compound BiCoPO5 monoclinic, P2(1)/n, a = 7.2470(1) Angstrom, b = 1 1.2851(2) Angstrom, c = 5.2260(1) Angstrom and beta = 107.843(1)degrees, Z = 4, was synthesised and structurally characterised by powder X-ray diffrac tion and infrared spectroscopy. It is isostructural with bismuth nickel oxy phosphate BiNiOPO4. The crystal structure is built from a complex tridimens ional assembly of (Co/Ni)(2)O-10 dimers linked by PO4 groups, This forms la rge tunnels running along c which host Bi3+ cations. Smaller tunnels runnin g along a and crossing the latter were also evidenced. It is noteworthy tha t the original BiNiPO5 lattice is appreciably increased with Co2+ cations a s the transition metal. This feature is essentially pointed out by the Co-O longer distances. The Bi3+ cation is surrounded by a strongly distorted ox ygen octahedron. Reducing the Bi-O bonds to the three shortest, Bi environm ent can be considered as tetrahedral considering the BiO(3)Lp polyhedron, L p = 6s(2) lone pair (Lp). The lone pair localisation was performed from ele ctrostatic interactions and revealed Lp - Bi distance of 0.68 Angstrom and 0.58 Angstrom, Tor Co2+ and Ni2+ compounds respectively. The infrared spect ra of the two compounds are essentially the same and only show slight shift s of the significant bands.