2013
DOI: 10.1063/1.4818335
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In situ Brillouin study of sodium alumino silicate glasses under pressure

Abstract: The in situ elastic and plastic behaviors of sodium aluminosilicate glasses with different degrees of depolymerization were analyzed using Brillouin spectroscopy. The observed elastic anomaly progressively vanished with depolymerization. The densification process appears to be different from that observed in pure silica glass. In the plastic regime of densified glasses hysteresis loops were observed and related to modification of the local silicon environment facilitated by the addition of sodium.

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Cited by 26 publications
(20 citation statements)
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“…[8a, 19] Raman spectroscopy,w ith the wavelength range 0-1200 cm À1 ,w as appliedt os crutinize the presence of Magneli phases.A st he outer layer of the sample was treated by HMDS, SiO 2 shells were introduced and accompanied by the appearance of characteristics SiO 2 peaks at 422 cm À1 . [20] In general, the E g anatase mode has an average peak position of 145.5 cm À1 ,t he E g rutile mode has an average peak positiono f 440.4 cm À1 ,a nd the A 1g rutile mode has an average peak position of 611.8 cm À1 . [21] The characteristic peak at 140 cm À1 and humps in this wavelength range are the signature of Magneli Ti 4 O 7 .…”
Section: Resultsmentioning
confidence: 99%
“…[8a, 19] Raman spectroscopy,w ith the wavelength range 0-1200 cm À1 ,w as appliedt os crutinize the presence of Magneli phases.A st he outer layer of the sample was treated by HMDS, SiO 2 shells were introduced and accompanied by the appearance of characteristics SiO 2 peaks at 422 cm À1 . [20] In general, the E g anatase mode has an average peak position of 145.5 cm À1 ,t he E g rutile mode has an average peak positiono f 440.4 cm À1 ,a nd the A 1g rutile mode has an average peak position of 611.8 cm À1 . [21] The characteristic peak at 140 cm À1 and humps in this wavelength range are the signature of Magneli Ti 4 O 7 .…”
Section: Resultsmentioning
confidence: 99%
“…Therefore, understanding the atomic structure (e.g., coordination numbers and degree of polymerization) of glasses upon compression is essential for understanding the pressure dependence of the macroscopic properties. The pressure-induced structural changes that occur include changes in the next-nearest neighbor (NNN) distributions and ring statistics (Lee, 2010;Sonneville et al, 2013), number of non-bridging oxygen (NBO) (Xue and Stebbins, 1993;George and Stebbins, 1996), atomic coordination number of network-former cations (Smedskjaer et al, 2014b), and network-former/modifier-oxygen bond distances (Xue and Stebbins, 1993;Sonneville et al, 2013).…”
Section: Pressure-induced Structural Changesmentioning
confidence: 99%
“…10(a)], in a good agreement with experimental observation. 44 The above results clearly show that it is such local beta-to alpha-ring transitions giving rise to the elastic softening upon initial compression in silica glass. Therefore, by eliminating localized ring conformation changes, the mechanical anomaly in silica glass can be completely eradicated.…”
Section: Tuning Elastic Anomaly Via Microscopic Structurementioning
confidence: 66%