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Structure of alkali borosilicate glasses and melts according to Raman spectroscopy data

Using the technique of high-temperature Raman scattering spectroscopy, we studied the structure of glasses and melts of the systems Na 2 O-B 2 O 3 -SiO 2 , K 2 O-B 2 O 3 -SiO 2 , and Cs 2 O-B 2 O 3 -SiO 2 with the relations (M = Na, K, Cs) and and 4/3. Based on the analysis of the registered spectra...

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Bibliographic Details
Published in:Glass physics and chemistry 2013-03, Vol.39 (2), p.105-112
Main Authors: Osipov, A. A., Osipova, L. M., Eremyashev, V. E.
Format: Article
Language:English
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Summary:Using the technique of high-temperature Raman scattering spectroscopy, we studied the structure of glasses and melts of the systems Na 2 O-B 2 O 3 -SiO 2 , K 2 O-B 2 O 3 -SiO 2 , and Cs 2 O-B 2 O 3 -SiO 2 with the relations (M = Na, K, Cs) and and 4/3. Based on the analysis of the registered spectra, we have shown that, at a high content of SiO 2 , the disordered network of glasses is composed of the Q 4 , Q 3 , [BO 4/2 ] − tetrahedrons and BO 3/2 triangles. When the content of SiO 2 reduces, asymmetric borate triangles BØ 2/2 O − are formed in the structure in addition. A substantial part of borate tetrahedrons are included into the content of mixed borosilicate rings composed of two silicon-oxygen and two boron-oxygen tetrahedrons. The amount of borate structural units joined into purely borate superstructural groups increases with a decrease of the silicon oxide content, depends on the alkali kation type, and grows in the direction from Cs to Na. An increase in the temperature causes a decrease of various types of rings and growth of the concentration of asymmetric triangles. Both in glasses and melts, the fraction of the BO 2/2 O − triangles depends on the alkali cation type and increases in the succession Cs → K → Na. The results obtained present the basis to suggest that there is some differentiation in the mechanisms of structural reconstruction of the glasses under study by their heating depending on the modifying oxide.
ISSN:1087-6596
1608-313X
DOI:10.1134/S1087659613020119