2018
DOI: 10.1140/epje/i2018-11662-3
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Structural-dynamical transition in the Wahnström mixture

Abstract: In trajectory space, dynamical heterogeneities in glass-forming liquids correspond to the emergence of a dynamical phase transition between an active phase poor in local structure and an inactive phase which is rich in local structure. We support this scenario with the study of a model additive mixture of Lennard-Jones particles, quantifying how the choice of the relevant structural and dynamical observable affects the transition in trajectory space. We find that the low mobility, structure-rich phase is domin… Show more

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Cited by 18 publications
(21 citation statements)
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References 70 publications
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“…Our results unambiguously demonstrate the existence of a discontinuous first-order phase transition in the ensemble of trajectories of polydisperse hard spheres between the normal liquid (low population of LFS and high mobility) and a non-equilibrium glassy phase (high population of LFS, the structural relaxation time exceeds the trajectory length). These results complement previous studies on two binary Lennard-Jones glass formers: Kob-Andersen [30,32,33,71] and Wahnström [71].…”
Section: Discussionsupporting
confidence: 91%
“…Our results unambiguously demonstrate the existence of a discontinuous first-order phase transition in the ensemble of trajectories of polydisperse hard spheres between the normal liquid (low population of LFS and high mobility) and a non-equilibrium glassy phase (high population of LFS, the structural relaxation time exceeds the trajectory length). These results complement previous studies on two binary Lennard-Jones glass formers: Kob-Andersen [30,32,33,71] and Wahnström [71].…”
Section: Discussionsupporting
confidence: 91%
“…Overall, our results are consistent with the idea that at least part of the dynamical slowdown is driven by the emergence of a set of locally favored structures, in agreement with earlier observations on these models (see, e.g., refs. 19 , 43 , 44 ). As the system is pushed closer to the glass transition, these structures become more stable, due to a more favorable local packing or potential energy, with a profound impact on both local and global dynamics 3 .…”
Section: Discussionmentioning
confidence: 99%
“…Bottom: Population n * = Z * /(1 + Z * ) of excited states, which drops below the onset temperature To. We normalize Z * (To) = 1. arXiv:1902.07768v1 [cond-mat.stat-mech] 20 Feb 2019 finds support from simulations of atomistic model glass formers [15,16] and colloid experiments [17].…”
Section: Introductionmentioning
confidence: 91%