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Original scientific paper

Bose Peak and Vibrational Bands in Raman Spectra of Sodium Borosilicate Glass

Vlasta Mohaček ; Ruđer Bošković Institute, P. P. Box 1016, 41000 Zagreb, Croatia
Krešimir Furić ; Ruđer Bošković Institute, P. P. Box 1016, 41000 Zagreb, Croatia

Fulltext: english, pdf (10 MB) pages 119-123 downloads: 267* cite
APA 6th Edition
Mohaček, V. & Furić, K. (1992). Bose Peak and Vibrational Bands in Raman Spectra of Sodium Borosilicate Glass. Croatica Chemica Acta, 65 (1), 119-123. Retrieved from https://hrcak.srce.hr/137266
MLA 8th Edition
Mohaček, Vlasta and Krešimir Furić. "Bose Peak and Vibrational Bands in Raman Spectra of Sodium Borosilicate Glass." Croatica Chemica Acta, vol. 65, no. 1, 1992, pp. 119-123. https://hrcak.srce.hr/137266. Accessed 21 Sep. 2021.
Chicago 17th Edition
Mohaček, Vlasta and Krešimir Furić. "Bose Peak and Vibrational Bands in Raman Spectra of Sodium Borosilicate Glass." Croatica Chemica Acta 65, no. 1 (1992): 119-123. https://hrcak.srce.hr/137266
Harvard
Mohaček, V., and Furić, K. (1992). 'Bose Peak and Vibrational Bands in Raman Spectra of Sodium Borosilicate Glass', Croatica Chemica Acta, 65(1), pp. 119-123. Available at: https://hrcak.srce.hr/137266 (Accessed 21 September 2021)
Vancouver
Mohaček V, Furić K. Bose Peak and Vibrational Bands in Raman Spectra of Sodium Borosilicate Glass. Croatica Chemica Acta [Internet]. 1992 [cited 2021 September 21];65(1):119-123. Available from: https://hrcak.srce.hr/137266
IEEE
V. Mohaček and K. Furić, "Bose Peak and Vibrational Bands in Raman Spectra of Sodium Borosilicate Glass", Croatica Chemica Acta, vol.65, no. 1, pp. 119-123, 1992. [Online]. Available: https://hrcak.srce.hr/137266. [Accessed: 21 September 2021]

Abstracts
The existence of an asymmetric broad band called boson (Bose) peak in W as well as in VH polarized Raman spectra of sodium borosilicate glass with various amounts of SnO is shown and its bandshape fitted according to the formula /v H — C(u>)g(io) where n(to) stands for Bose-Einstein occupation number and C(m)g(m) is given by C(u>)g(a>) =
Parameter On addition of SnO (1.5 to 10 wt %) the shape of boson peak in VH spectra changes on addition of 1.5 wt %, but remains unchanged on further addition of SnO. In the W - 4/3 VH spectrum, a new peak around 530 cm-1 appears, indicating that tin ions behave as network formers.

Hrčak ID: 137266

URI
https://hrcak.srce.hr/137266

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