The Brillouin elastic free energy change ΔΦ between thermally annealed and quenched (Na2O)x(SiO2)1−x glasses is found to increase linearly for x>0.23 (floppy phase), and to nearly vanish at x 0.23, but to nearly vanish in the 0.18<x<0.23 range, suggesting the existence of an intermediate phase between the floppy and stressed-rigid phases.
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Vaills et al. (2005) studied this question.
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