2002
DOI: 10.1209/epl/i2002-00470-4
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Elastic properties of a-SiO 2 up to 2300 K from Brillouin scattering measurements

Abstract: The velocities of the transverse and longitudinal acoustic modes of silica glass and liquid have been measured by Brillouin spectroscopy from 300 to 2300 K. Elastic properties of liquid SiO2 could thus be studied over an interval of 800 K above the standard glass transition temperature. The velocity of the transverse mode, and thus the shear modulus, first increases with temperature and then decreases after reaching a maximum near the glass transition temperature. The velocity of the longitudinal mode and the … Show more

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Cited by 129 publications
(98 citation statements)
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“…The data of Fig. 2b are close to previous determination of the literature in several commercial silica samples, 21,22,23 and the high temperature part of those curves will be also discussed, in comparison with previous determinations, in another article (Ref. 24).…”
Section: 12supporting
confidence: 88%
“…The data of Fig. 2b are close to previous determination of the literature in several commercial silica samples, 21,22,23 and the high temperature part of those curves will be also discussed, in comparison with previous determinations, in another article (Ref. 24).…”
Section: 12supporting
confidence: 88%
“…23 The variation of the sound velocity with temperature is found to be comparable to that determined by means of Brillouin light scattering (BLS). 36 Using the resulting Debye frequency we show that the temperature dependence of the BP in silica does not follow the elastic medium transformation, confirming the observation of Ref. 20.…”
Section: Introductionsupporting
confidence: 83%
“…By comparing the sound speeds in Table I, it is clear that the low-frequency DOS of our models for a-Si and a-SiO 2 are dominated by transverse modes, which is expected due to their degeneracy and lower frequencies compared to the longitudinal modes. The transverse sound speed predicted for our model of a-SiO 2 is 85% of that predicted by the other methods (Table I) and that measured by experiment [63,67,70], which is likely related to the larger density of our samples (see Sec. III A).…”
Section: Sound Speedmentioning
confidence: 46%
“…The smaller values predicted by the structure factors and DOS result from the concavedown dispersion seen at low wave vector (i.e., we are not able to reach the linear portion of the dispersion curve). Experimental measurements of the sound speeds of a-SiO 2 using Brillouin light and inelastic x-ray scattering range between 3800 to 4000 m/s (transverse) and 6000 to 6400 m/s (longitudinal) [63,67,70]. Differences between our predictions and experimental measurements may be related to limitations of the BKS potential.…”
Section: Sound Speedmentioning
confidence: 67%