Unified Theory of Activated Relaxation in Liquids over 14 Decades in Time
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We formulate a predictive theory at the level of forces of activated relaxation in hard sphere fluids and thermal liquids that covers in a unified manner the apparent Arrhenius, crossover and deeply supercooled regimes. The alpha relaxation event involves coupled cage-scale hopping and a long range collective elastic distortion of the surrounding liquid, which results in two inter-related, but distinct, barriers. The strongly temperature and density dependent collective barrier is associated with a growing length scale, the shear modulus and density fluctuations. Thermal liquids are mapped to an effective hard sphere fluid based on matching long wavelength density fluctuation amplitudes, resulting in a zeroth order quasi-universal description. The theory is devoid of fit parameters, has no divergences at finite temperature nor below jamming, and captures the key features of the alpha time of molecular liquids from picoseconds to hundreds of seconds.
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Cited by 2 Pith papers
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Non-Maxwellian Velocity Statistics in Supercooled Liquids and Their Possible Relation to Super-Arrhenius Viscosity
Supercooled liquids exhibit persistent non-Maxwellian velocity distributions with excess kurtosis 0<κ≲0.3 linked via temperature fluctuation width A_bar≈0.08 to super-Arrhenius viscosity across 45 glass formers.
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Non-Maxwellian Velocity Statistics in Supercooled Liquids and Their Possible Relation to Super-Arrhenius Viscosity
Supercooled liquids exhibit persistent non-Maxwellian velocity distributions with excess kurtosis linked to temperature fluctuation width A-bar ~0.08, consistent with viscosity data collapse across 45 glass formers.
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