2013
DOI: 10.1134/s1087659613020119
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Structure of alkali borosilicate glasses and melts according to Raman spectroscopy data

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Cited by 50 publications
(58 citation statements)
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“…It should be noted that a danburite structure of CaO•B2O3•2SiO2 (one BO4 -unit is surrounded by three SiO4 and one BO4 -) was not considered which is observed around 630 cm -1 of Raman shift. 40) According to Osipov et al, 42) a danburite spectrum is observed at 614 cm -1 with a complete absence of peaks within the 1 400-1 500 cm -1 range, however, spectra within the range were found almost the entire compositions in the current study. In addition, a fully-polymerized tetrahedral silicate (SiO4) unit, which is an essential component for danburite, was rarely observed.…”
Section: Effect Of Temperature and Composition On Thermal Conductivitycontrasting
confidence: 36%
“…It should be noted that a danburite structure of CaO•B2O3•2SiO2 (one BO4 -unit is surrounded by three SiO4 and one BO4 -) was not considered which is observed around 630 cm -1 of Raman shift. 40) According to Osipov et al, 42) a danburite spectrum is observed at 614 cm -1 with a complete absence of peaks within the 1 400-1 500 cm -1 range, however, spectra within the range were found almost the entire compositions in the current study. In addition, a fully-polymerized tetrahedral silicate (SiO4) unit, which is an essential component for danburite, was rarely observed.…”
Section: Effect Of Temperature and Composition On Thermal Conductivitycontrasting
confidence: 36%
“…of the ISG makes the unambiguous assignment of Raman bands to specific structural units difficult. Its Raman spectrum has the following general features of sodium borosilicate glasses [33,34]: 1) the main band around 500 cm −1 corresponds to the bridging oxygen vibration of the SiO 4 network; 2) the peak around 630 cm −1 is attributed to the breathing mode of borosilicate rings (possibly "loose BO 3 "); 3) the broad peak in the range of 850 to 1200 cm −1 is due to the symmetric stretching vibration of Si-O bonds in Q n species of SiO 4 tetrahedra (1 b n b 4 bridging oxygen); and 4) the weak peak in the region from 1200 to 1550 cm − 1 arises from B-O bond vibration of BO 3 and BO 4 units. Significant intensity changes are seen in the peak around 630 cm −1 and in the broad peak around 950-980 cm −1 , both decrease at and above 600°C.…”
Section: Discussionmentioning
confidence: 99%
“…Both the relative intensity and the shape of the Raman profile from 1000 to 1250 cm −1 are very similar to those observed for SiO 2 , suggesting that the connectivity of the silicate sub-network in KBS resembles that in silica glass as manifested also by infrared spectroscopy. The small intensity build up between 1060 and 1200 cm −1 suggests a very small content of Q 3 silicate tetrahedral units, as their characteristic silicon-oxygen stretching vibration is expected in this frequency range [39,[46][47][48]. It should be noted that the Raman cross section of the stretching modes associated to tetrahedral with NBOs, such as Q 3 groups, is much higher compared to that of fully polymerized Q 4 units.…”
Section: Raman Spectroscopy Of Pristine Glassesmentioning
confidence: 98%
“…The content of trigonal borate units in glass NBS1 should be limited judging by the very weak activity in the 1300 to 1600 cm −1 range, which is in line with the corresponding infrared data. The strong feature of the NBS1 glass spectrum at 1070 cm − 1 shows clearly the presence of Q 3 silicate tetrahedra, while the shoulders at~1150 and 950 cm − 1 are associated with silicate units Q 4 and Q 2 , respectively [46][47][48].…”
Section: Raman Spectroscopy Of Pristine Glassesmentioning
confidence: 99%