We investigate the dynamics of polydisperse hard spheres at high packing fractions [curly or open phi]. We use extensive numerical simulations based on an experimentally-realistic particle size distribution (PSD) and compare to commonly-used PSDs such as Gaussian or top hat distribution. We find that the mode of kinetic arrest depends on the PSD's shape and not only on its variance. For the experimentally-realistic PSD we find ageing dynamics even though the density correlators decay fully to zero for [curly or open phi] ? 0.59. We observe substantial decoupling of the dynamics of the smallest and largest particles. While the smallest particles remain diffusive in all our simulations, a power-law describes the largest-particle diffusion, suggesting an ideal arrest at [curly or open phi]c [similar] 0.588. The latter is however averted just before [curly or open phi]c, due to the presence of the mobile smallest particles. In addition, we identify that a partial aging mechanism is at work, whose effects are most pronounced for the largest particles. By comparing our results with recent experimental observations of ergodic behavior up to [curly or open phi] [similar] 0.6 in a hard-sphere system, we argue that this is an effect of polydispersity, which smears out the glass transition.

On polydispersity and the hard sphere glass transition

Emanuela Zaccarelli;
2015

Abstract

We investigate the dynamics of polydisperse hard spheres at high packing fractions [curly or open phi]. We use extensive numerical simulations based on an experimentally-realistic particle size distribution (PSD) and compare to commonly-used PSDs such as Gaussian or top hat distribution. We find that the mode of kinetic arrest depends on the PSD's shape and not only on its variance. For the experimentally-realistic PSD we find ageing dynamics even though the density correlators decay fully to zero for [curly or open phi] ? 0.59. We observe substantial decoupling of the dynamics of the smallest and largest particles. While the smallest particles remain diffusive in all our simulations, a power-law describes the largest-particle diffusion, suggesting an ideal arrest at [curly or open phi]c [similar] 0.588. The latter is however averted just before [curly or open phi]c, due to the presence of the mobile smallest particles. In addition, we identify that a partial aging mechanism is at work, whose effects are most pronounced for the largest particles. By comparing our results with recent experimental observations of ergodic behavior up to [curly or open phi] [similar] 0.6 in a hard-sphere system, we argue that this is an effect of polydispersity, which smears out the glass transition.
2015
Istituto dei Sistemi Complessi - ISC
sphere glass transition
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/258390
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