Abstract

In many glass-forming liquids, fractional Stokes-Einstein relation (SER) is observed above the glass transition temperature. However, the origin of such phenomenon remains elusive. Using molecular dynamics simulations, we investigate the break- down of SER and the onset of fractional SER in a model of metallic glass-forming liquid. We find that SER breaks down when the size of the largest cluster consisting of trapped atoms starts to increase sharply at which the largest cluster spans half of the simulations box along one direction, and the fractional SER starts to follows when the largest cluster percolates the entire system and forms 3-dimentional network structures. Further analysis based on the percolation theory also confirms that percolation occurs at the onset of the fractional SER. Our results directly link the breakdown of the SER with structure inhomogeneity and onset of the fraction SER with percolation of largest clusters, thus provide a possible picture for the break- down of SER and onset of fractional SER in glass-forming liquids, which is is important for the understanding of the dynamic properties in glass-forming liquids.

Highlights

  • The Stokes-Einstein relation (SER) describes the relation between diffusion constant D and structural relaxation time τ1,2, which follows D ∝(τ/T)−1 at high temperature T

  • Using classical molecular dynamics (MD) simulations, we study the breakdown of SER and onset of fractional SER in a model of metallic glass-forming liquid, Cu64Zr36

  • We first investigate the dynamic properties of the liquid

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Summary

Introduction

The Stokes-Einstein relation (SER) describes the relation between diffusion constant D and structural relaxation time τ1,2, which follows D ∝(τ/T)−1 at high temperature T. Using classical molecular dynamics (MD) simulations, we study the breakdown of SER and onset of fractional SER in a model of metallic glass-forming liquid, Cu64Zr36. We observe the breakdown of SER in the metallic liquid, from normal SER with ξ = 1 at high temperatures to fractional SER with ξ = 0.67 at low temperatures. This breakdown is correlated with the change in the local structures characterized by the size of the largest cluster www.nature.com/scientificreports/. At lower temperatures where the fractional SER follows, the largest cluster percolates the entire system and forms a 3-dimensional network structure. Our results link the SER and fractional SER with structure heterogeneity, provide a possible picture for the breakdown of SER and onset of fractional SER in glass-forming liquids

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