2010
DOI: 10.1007/978-1-4419-7649-9_2
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Glass-Forming Substances and Systems

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Cited by 3 publications
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“…However, the knowledge for the mixing behaviors is mainly based on indirect measurements using properties such as heat of mixing Δ H mix , reflecting the interactions between the unlike species, , or, dynamically, the width relaxation profile gauged by the non-exponential factor (or stretching exponent) β KWW (0 < β KWW ≤ 1) of structural α relaxation, which is crucial to address the dynamic heterogeneity in glasses and supercooled liquids . The dynamic parameter can be obtained by fitting the α-relaxation dispersion using the Kohlrausch–Williams–Watts (KWW) function, ϕ­( t ) = exp­[−( t /τ α ) β KWW ], where τ α is the relaxation time. , However, the quantitative relationship between the two parameters and the concentration fluctuations has not been available, and direct access to concentration fluctuations in mixing systems with higher accuracy still remains to be clarified.…”
mentioning
confidence: 99%
“…However, the knowledge for the mixing behaviors is mainly based on indirect measurements using properties such as heat of mixing Δ H mix , reflecting the interactions between the unlike species, , or, dynamically, the width relaxation profile gauged by the non-exponential factor (or stretching exponent) β KWW (0 < β KWW ≤ 1) of structural α relaxation, which is crucial to address the dynamic heterogeneity in glasses and supercooled liquids . The dynamic parameter can be obtained by fitting the α-relaxation dispersion using the Kohlrausch–Williams–Watts (KWW) function, ϕ­( t ) = exp­[−( t /τ α ) β KWW ], where τ α is the relaxation time. , However, the quantitative relationship between the two parameters and the concentration fluctuations has not been available, and direct access to concentration fluctuations in mixing systems with higher accuracy still remains to be clarified.…”
mentioning
confidence: 99%