2008
DOI: 10.1016/j.jssc.2008.06.011
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Consolidated silica glass from nanoparticles

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Cited by 49 publications
(42 citation statements)
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“…The peaks at 1102 and 472 cm −1 are visible, being related to the asymmetric Si-O-Si stretching vibration and Si-O-Si bending vibration, respectively [28]. These results are also consistent with the XRD.…”
Section: Structural Features Of the Solids By Ftirsupporting
confidence: 85%
See 1 more Smart Citation
“…The peaks at 1102 and 472 cm −1 are visible, being related to the asymmetric Si-O-Si stretching vibration and Si-O-Si bending vibration, respectively [28]. These results are also consistent with the XRD.…”
Section: Structural Features Of the Solids By Ftirsupporting
confidence: 85%
“…Further, these results are consistent with the TG analysis. As the contribution of hydroxyl absorption due to physisorbed water is expected to be small, the aforementioned band may be assigned to the hydrogen bonded hydroxyl groups of Si-OH, Al-OH, Zr-OH or Ti-OH [27,28]. This is a good indication of the elimination of the organic precursors to form the nanostructured phases of the oxides mentioned by XRD.…”
Section: Porosity Studiesmentioning
confidence: 99%
“…Protons within inorganic structures devoid of significant internal motions still relax much faster than notoriously slowly relaxing spin-1/2 nuclei in glasses (e.g., 29 Si, 31 P, 13 C, and 89 Y), normally allowing for using 1 H relaxation delays <10 s. Nevertheless, cases do exist where very long pulse delays are required. One example is Si-O 1 H moieties present in very low amounts in vitreous SiO 2 , for which we have encountered T 1 % 190 s, which if using 90°excitation pulses would require 16 min relaxation delays in the signal averaging to ensure a quantitative 1 H NMR spectrum [156].…”
Section: T 1 Relaxation and Pulse Delaysmentioning
confidence: 98%
“…Silica gives a strong phonon-polariton signal between about 1050 and 1300 cm −1 . The main oscillator is located at about 1070 cm −1 , which is at the same time the wavenumber of the so-called transversal optical (TO) phonon [85]. The corresponding dip of the 3 nm SiO 2 layer did not appear in proximity to the TO wavenumber, but instead, closer to the longitudinal optical (LO) phonon at about 1250 cm −1 in the range of the Fuchs-Kliewer surface phonon polariton.…”
Section: Linear Nanoantennasmentioning
confidence: 96%