Details
| Original language | English |
|---|---|
| Pages (from-to) | 91-103 |
| Number of pages | 13 |
| Journal | Journal of Non-Crystalline Solids |
| Volume | 240 |
| Issue number | 1-3 |
| Publication status | Published - 2 Oct 1998 |
Abstract
Incorporation mechanisms of H2 in silica glass were studied with Raman and infrared (IR) microspectroscopy. Hydrogenated samples were prepared at temperatures between 800°C and 955°C at 2 kbar total pressure. Hydrogen fugacities (fH2) were controlled using the double capsule technique with the iron-wüstite (IW) buffer assemblage generating fH2 of 1290-1370 bars corresponding to H2 partial pressures (PH2) of 960-975 bars. We found that silica glass hydrogenated under such conditions contains molecular hydrogen (H2) in addition to SiH and SiOH groups. H2 molecules dissolved in the quenched glasses introduce a band at 4136 cm-1 in the Raman spectra which in comparison to that of gaseous H2 is wider and is shifted to lower frequency. IR spectra of hydrogenated samples contain a band at 4138 cm-1 which we assign to the stretching vibration of H2 molecules located in non-centrosymmetric sites. The Raman and IR spectra indicate that the dissolved H2 molecules interact with the silicate network. We suggest that the H2 band is the envelope of at least three components due to the occupation of at least three different interstitial sites by H2 molecules. Both, Raman and IR spectra of hydrogenated glasses contain bands at ∼2255 cm-1 which may be due to the vibration of SiH groups. Under the assumption that the reaction Si-O-Si + H2 → Si-H + Si-O-H describes adequately the 'chemical dissolution' of H2 molecules, the SiH concentrations in our samples were determined and the molar extinction coefficient for the SiH absorption band in the infrared (ε2255(SiH)) could then be estimated to be 45 ± 3 1/mol cm. The solubility of molecular H2 in our hydrogenated samples was determined using the IR absorption band at 4138 cm-1 and the extinction coefficient given by Shelby [J. Non-Cryst. Solids 179 (1994) 138]. Samples quenched with different cooling rates gave nearly identical Raman and IR spectra, suggesting that the chemical dissolution of hydrogen (SiH and SiOH) can be quenched to room temperature without changing relative concentrations and that no exsolution of hydrogen occurred during the quench.
ASJC Scopus subject areas
- Materials Science(all)
- Electronic, Optical and Magnetic Materials
- Materials Science(all)
- Ceramics and Composites
- Physics and Astronomy(all)
- Condensed Matter Physics
- Materials Science(all)
- Materials Chemistry
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In: Journal of Non-Crystalline Solids, Vol. 240, No. 1-3, 02.10.1998, p. 91-103.
Research output: Contribution to journal › Article › Research › peer review
}
TY - JOUR
T1 - Incorporation of H2 in vitreous silica, qualitative and quantitative determination from Raman and infrared spectroscopy
AU - Schmidt, Burkhard C.
AU - Holtz, Francois
AU - Bény, Jean M.
N1 - Funding Information: This research constituted a part of B.C.S.'s PhD thesis, supported by a grant of the French Ministry for Research and Education. The manuscript benefited from the critical comments of two anonymous reviewers. Copyright: Copyright 2018 Elsevier B.V., All rights reserved.
PY - 1998/10/2
Y1 - 1998/10/2
N2 - Incorporation mechanisms of H2 in silica glass were studied with Raman and infrared (IR) microspectroscopy. Hydrogenated samples were prepared at temperatures between 800°C and 955°C at 2 kbar total pressure. Hydrogen fugacities (fH2) were controlled using the double capsule technique with the iron-wüstite (IW) buffer assemblage generating fH2 of 1290-1370 bars corresponding to H2 partial pressures (PH2) of 960-975 bars. We found that silica glass hydrogenated under such conditions contains molecular hydrogen (H2) in addition to SiH and SiOH groups. H2 molecules dissolved in the quenched glasses introduce a band at 4136 cm-1 in the Raman spectra which in comparison to that of gaseous H2 is wider and is shifted to lower frequency. IR spectra of hydrogenated samples contain a band at 4138 cm-1 which we assign to the stretching vibration of H2 molecules located in non-centrosymmetric sites. The Raman and IR spectra indicate that the dissolved H2 molecules interact with the silicate network. We suggest that the H2 band is the envelope of at least three components due to the occupation of at least three different interstitial sites by H2 molecules. Both, Raman and IR spectra of hydrogenated glasses contain bands at ∼2255 cm-1 which may be due to the vibration of SiH groups. Under the assumption that the reaction Si-O-Si + H2 → Si-H + Si-O-H describes adequately the 'chemical dissolution' of H2 molecules, the SiH concentrations in our samples were determined and the molar extinction coefficient for the SiH absorption band in the infrared (ε2255(SiH)) could then be estimated to be 45 ± 3 1/mol cm. The solubility of molecular H2 in our hydrogenated samples was determined using the IR absorption band at 4138 cm-1 and the extinction coefficient given by Shelby [J. Non-Cryst. Solids 179 (1994) 138]. Samples quenched with different cooling rates gave nearly identical Raman and IR spectra, suggesting that the chemical dissolution of hydrogen (SiH and SiOH) can be quenched to room temperature without changing relative concentrations and that no exsolution of hydrogen occurred during the quench.
AB - Incorporation mechanisms of H2 in silica glass were studied with Raman and infrared (IR) microspectroscopy. Hydrogenated samples were prepared at temperatures between 800°C and 955°C at 2 kbar total pressure. Hydrogen fugacities (fH2) were controlled using the double capsule technique with the iron-wüstite (IW) buffer assemblage generating fH2 of 1290-1370 bars corresponding to H2 partial pressures (PH2) of 960-975 bars. We found that silica glass hydrogenated under such conditions contains molecular hydrogen (H2) in addition to SiH and SiOH groups. H2 molecules dissolved in the quenched glasses introduce a band at 4136 cm-1 in the Raman spectra which in comparison to that of gaseous H2 is wider and is shifted to lower frequency. IR spectra of hydrogenated samples contain a band at 4138 cm-1 which we assign to the stretching vibration of H2 molecules located in non-centrosymmetric sites. The Raman and IR spectra indicate that the dissolved H2 molecules interact with the silicate network. We suggest that the H2 band is the envelope of at least three components due to the occupation of at least three different interstitial sites by H2 molecules. Both, Raman and IR spectra of hydrogenated glasses contain bands at ∼2255 cm-1 which may be due to the vibration of SiH groups. Under the assumption that the reaction Si-O-Si + H2 → Si-H + Si-O-H describes adequately the 'chemical dissolution' of H2 molecules, the SiH concentrations in our samples were determined and the molar extinction coefficient for the SiH absorption band in the infrared (ε2255(SiH)) could then be estimated to be 45 ± 3 1/mol cm. The solubility of molecular H2 in our hydrogenated samples was determined using the IR absorption band at 4138 cm-1 and the extinction coefficient given by Shelby [J. Non-Cryst. Solids 179 (1994) 138]. Samples quenched with different cooling rates gave nearly identical Raman and IR spectra, suggesting that the chemical dissolution of hydrogen (SiH and SiOH) can be quenched to room temperature without changing relative concentrations and that no exsolution of hydrogen occurred during the quench.
UR - http://www.scopus.com/inward/record.url?scp=0032475562&partnerID=8YFLogxK
U2 - 10.1016/S0022-3093(98)00698-X
DO - 10.1016/S0022-3093(98)00698-X
M3 - Article
AN - SCOPUS:0032475562
VL - 240
SP - 91
EP - 103
JO - Journal of Non-Crystalline Solids
JF - Journal of Non-Crystalline Solids
SN - 0022-3093
IS - 1-3
ER -