Abstract

THREE structures have been proposed for high cristobalite, which exists for T⪞273° C in pure, well-ordered material. These have been described by Wyckoff1 and by Sosman2 who suggests that all three might be correct for different specimens. The first investigation, by Wyckoff3,4 himself, from powder photographs taken at 290 and 430° C on a specimen prepared by devitrifying vitreous silica at 1,560° C, placed the structure in space group Fd3m, with 8[SiO2] per unit cell. The Si atoms form a diamond lattice with the oxygens lying along the lines-of-centres between adjacent silicas. This structure is often still described in textbooks as the structure of real, or sometimes of “ideal”, cristobalite (see refs 5-7). It cannot be correct, however, because it requires an Si-O-Si angle of 180° and an Si-O bond length of 1.54 Å, both of which differ considerably from values established for other forms of silica, where Si-O = 1.61 ± 0.02 Å and , and for silicates, where usually Si-O > 1.58 Å and .
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References
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LEADBETTER, A., SMITH, T. & WRIGHT, A. Structure of High Cristobalite. Nature Physical Science 244, 125–126 (1973). https://doi.org/10.1038/physci244125a0
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DOI: https://doi.org/10.1038/physci244125a0
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