Issue 17, 1997

Vibrational modes and structure of rare earth halide–alkali halide binary melts

YBr3–ABr (A = Li, K, Cs) and YF3–KF

Abstract

Raman spectra of the following binary molten salt systems have been measured: (a) YBr 3 –ABr (A = Li, K, Cs) at temperatures up to 920 °C and at different compositions; (b) YF 3 –KF at temperatures up to 1000 °C and compositions up to 50% YF 3 . The spectral changes occurring upon melting of Cs 2 NaYBr 6 , YBr 3 and K 3 YF 6 crystalline compounds were also measured. The data indicate that, in mixtures rich in alkali halide, YX 6 3− (X = F, Br) octahedra are the predominant species giving rise to two main bands P 1 (polarized) and D 1 (depolarized) which are assigned as follows: (a) YBr 6 3- , P 1 = 156 cm −1 , ν 1 (A 1g ) and D 1 = 78 cm −1 , ν 5 (F 2g ); and (b) YF 6 3− , P 1 = 445 cm −1 , ν 1 (A 1g ) and D 1 = 225 cm −1 , ν 5 (F 2g ). In molten mixtures rich in YBr 3 in addition to the P 1 and D 1 bands a new depolarized D 2 (ca. 210 cm −1 ) and a strong new polarized P 2 band appear in the spectra. The P 2 band shifts from ca. 200 cm −1 to ca. 250 cm −1 with increasing YBr 3 content. The presence of these four bands and their polarization characteristics suggest that the predominant vibrational modes in the YBr 3 -rich mixtures are due to a close C pyramidal like ‘unit’ arising from the D 3 distortions of the YBr 6 3− octahedra bound by edges in the melt. This behaviour, as well as the spectral changes upon melting YBr 3 , supports the view that the structure of pure molten YBr 3 consists of edge-sharing distorted octahedra. The molten fluoride mixtures YF 3 –KF at composition X YF3 > 0.25 also show four bands, two depolarized at ca. 240 cm −1 (D 1 ), ca. 370 cm −1 (D 2 ) and two overlapping polarized bands at ca. 440 cm −1 (P 1 ), ca. 460 cm −1 (P 2 ). Finally, the trends of the YX 3 –KX spectra on going from the bromide to chloride to fluoride melts suggest that pure molten YF 3 is likely to possess a loose ‘network’ structure of edge-bridged distorted octahedra as in the case of molten YCl 3 and YBr 3 .

Article information

Article type
Paper

J. Chem. Soc., Faraday Trans., 1997,93, 3081-3088

Vibrational modes and structure of rare earth halide–alkali halide binary melts

V. Dracopoulos, B. Gilbert, B. Brrensen, G. M. Photiadis and G. N. Papatheodorou, J. Chem. Soc., Faraday Trans., 1997, 93, 3081 DOI: 10.1039/A701864I

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