PHASE RELATIONS IN Y1-xSr 2+1.5xF7 ( -1.0 x 0.5) SYSTEM

Avesh K. Tyagi , Sadiqua J. Patwe and Nagabhusan S. Achary

Applied Chemistry Division, Bhabha Atomic Research Centre, Trombay, Mumbai 400 085, India
email:
sichem@magnum.barc.ernet.in

Keywords: Fluorides, X-ray diffraction, Phase relations

A series of mixed fluorides of general formula Y1-xSr2+1.5xF7 (x = -1.0< x< 0.5) was synthesized. The change in the crystal symmetry was systematically followed by powder XRD. It was found that up to Y0.7Sr2.45F7 the parent fluorite lattice was retained but after this composition and up to Y0.9Sr2.15F7 a mild tetragonal distortion was observed whereas stoichiometric YSr2F7 showed splitting of all the major peaks resulting into a large tetragonal unit cell. After the composition YSr2F7, further addition of YF3 to give compositions such as Y1.1Sr1.85F7, Y1.3Sr1.55F7, Y1.4Sr1.40F7, Y1.5Sr1.25F7, Y1.8Sr0.80F7, Y2Sr0.5F7 was also attempted. It was found that the doublets of the stoichiometric phase (YSr2F7) start merging. This feature was persistent in Y1.1Sr1.85F7 and Y1.2Sr1.70F7 which were found to have a cubic unit cell with 'a' = 11.4110±003 and 11.4350±005 A respectively. Futher addtion of YF3 to Y1.2Sr1.70F7 led to phase separation into two phases. These two phases could be observed at and after the nominal composition Y1.3Sr1.55F7. It was found that one set of new lines which started appearing at and beyond this nominal composition match very well with compound Y2Sr0.5F7, which was synthesized independently and indexed on a hexagonal LaF3 (tysonite) type cell with parameters 'a' = 6.882±0.002 A, 'c' = 7.032±0.003 A. Another phase could be indexed on a rhombohedral cell with lattice parameter 'a' = 8.9940±002 A and 'a' = 107.3° which is similar (1) to a rhombohedral supercell observed for Ca7+dY6-dF32-d (d = 0.475). It was found by us that the dissolution of YF3 up to 22 m% does not cause any noticeable distortion of the fluorite lattice unlike the obsevation of Sobolev et al (2) who found that about 41 m% of YF3 can be retained in the SrF2 lattice without causing any distortion. This difference between solubility limit of YF3 in SrF2 could be due to the difference in heat treatment as Sobolev et al quenched the samples from high temperature whereas ours were slow cooled samples. This implies that more and more YF3 can be retained in SrF2 lattice at higher temperature. The existence of YSr2F7 in this system was observed unequivocally which was shown to have a fluorite type superlattice somewhat similar to that in the compounds Ca2HoF7, Ca2TmF7 and Ca2YbF7 (3).

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