CHARACTERIZATION OF THE NONSTOICHIOMETRY IN LANTHANUM OXYFLUORIDE BY FT-IR ABSORPTION, RAMAN-SCATTERING, X-RAY-POWDER DIFFRACTION AND THERMAL-ANALYSIS

Citation
J. Holsa et al., CHARACTERIZATION OF THE NONSTOICHIOMETRY IN LANTHANUM OXYFLUORIDE BY FT-IR ABSORPTION, RAMAN-SCATTERING, X-RAY-POWDER DIFFRACTION AND THERMAL-ANALYSIS, Polyhedron, 16(19), 1997, pp. 3421-3427
Citations number
28
Categorie Soggetti
Chemistry Inorganic & Nuclear",Crystallography
Journal title
ISSN journal
02775387
Volume
16
Issue
19
Year of publication
1997
Pages
3421 - 3427
Database
ISI
SICI code
0277-5387(1997)16:19<3421:COTNIL>2.0.ZU;2-9
Abstract
The FT-IR absorption, FT-Raman scattering, X-ray powder diffraction (X PD), and thermogravimetry were used to explore the non-stoichiometry i n LaOF. The TGA-DTA analyses between 30 and 1500 degrees C showed that the LaO1-xF1+2x phases yielded the stoichiometric LaOF as an intermed iate product. The temperature of formation of the LaOF and La2O3 incre ased with increasing excess of fluoride.The room temperature XPD data in 6.5 less than or equal to 2 theta less than or equal to 121 degrees range were analyzed by the Rietveld profile refinement method and sub sequently by the bond valence calculations. All LaO1-xF1+2x phases pos sess the tetragonal PbFCl-type structure (space group: P4/nmm; Z = 2) while the stoichiometric LaOF has the hexagonal SmSI-type structure (s pace group: R (3) over bar m; Z = 6). The unit cell parameters a and c as well as the global instability index (GII) values increased with i ncreasing excess fluoride. The GII value for each LaO1-xF1+2x exceeded the limit (ca 0.2) for a possible breakdown of the tetragonal structu re indicating the inherent instability of these phases. The room tempe rature FTIR and FT-Raman spectra between 100 and 500 cm(-1) and 50 and 1000 cm(-1), respectively, were investigated using the factor group a nalysis to get more information of the local structure in LaOF. All fo ur IR modes (2A(2u)+ 2E(u)) for the both forms and five of the six Ram an modes (3A(1g)+ 3E(g) and A(1g)+ 2B(1g)+ 3E(g)) for the hexagonal an d the tetragonal form, respectively, were observed. The Raman spectra of the tetragonal LaOCl and all LaO1-xF1+2x were found remarkable simi lar. (C) 1997 Elsevier Science Ltd.