1991
DOI: 10.1016/0022-3093(91)90098-q
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The structure of some simple amorphous network solids revisited

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Cited by 108 publications
(39 citation statements)
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“…58 At all temperatures and for all phases, almost every Si atom is fourfold coordinated and almost every O atom is twofold coordinated, in agreement with experimental data. 43,44 Above T m during heating and above T g during cooling, the mean-square displacement of atoms grows linearly with the number of MC steps, showing that the motion of atoms is unbound, consistently with liquidlike diffusion. Comparison of atomic mobilities computed by MC during cooling to experimental data for the diffusion coefficient in disordered silica phases allows us to establish a rough correspondence with a real time scale.…”
Section: Summary Of Results For Bulk Siomentioning
confidence: 95%
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“…58 At all temperatures and for all phases, almost every Si atom is fourfold coordinated and almost every O atom is twofold coordinated, in agreement with experimental data. 43,44 Above T m during heating and above T g during cooling, the mean-square displacement of atoms grows linearly with the number of MC steps, showing that the motion of atoms is unbound, consistently with liquidlike diffusion. Comparison of atomic mobilities computed by MC during cooling to experimental data for the diffusion coefficient in disordered silica phases allows us to establish a rough correspondence with a real time scale.…”
Section: Summary Of Results For Bulk Siomentioning
confidence: 95%
“…At ambient temperature, they agree at least qualitatively and, to a large extent, semiquantitatively with experimental data provided by x-ray and neutron diffractions. 43,44 …”
Section: Summary Of Results For Bulk Siomentioning
confidence: 99%
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“…is found to be appreciable only in the small-k region, up to and including the main peak at kr I .~ (5/2)~r [6]. This remains true when the (narrow) Gaussians are replaced by ~-functions (which only eliminates a small damping, whose effect is negligible in the k-range of interest), and applies afortiori when S(k)s are compared, rather than F(k)s. Thus, in the case of vitreous SiO 2, the shape of the interference function beyond the main peak is rather well reproduced by a sum of two sines, n 1 sin kr 1 + n 2 sin kr2, with r2/r I = 2V~-/3.…”
Section: Structure Factor and Topological Short Range Ordermentioning
confidence: 79%
“…9). This choice is supported by the fact that the experimental results in neutron scattering factor of silica can be better fitted with a Lorentzian function than with a Gaussian one 63 . It should be noted that the fit has been done on the low Q part of the FSDP to avoid the contribution of the following peaks.…”
Section: First Sharp Diffraction Peakmentioning
confidence: 99%