2017/05/31 by Matthieu Wyart, Michael E. Cates · 6 citations
Materials Science · Physics and Astronomy · #Condensed matter physics #Coupling (piping) #Diffusion #Energy landscape #Glass properties and applications #Glass transition #Length scale #Material Dynamics and Properties #Materials science #Nuclear magnetic resonance #Physics #Polymer #Quantum mechanics #Relaxation (psychology) #Scale (ratio) #Slowdown #Statistical physics #Swap (finance) #Theoretical and Computational Physics #Thermodynamics #cond-mat.dis-nn
paper · pdf · doi:10.1103/physrevlett.119.195501
published as Phys. Rev. Lett. 119, 195501 (2017)
arxiv created 2017/09/28 · openalex publication_date 2017/11/09 · arxiv updated 2017/11/15 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/06
Several theories of the glass transition propose that the structural relaxation time τα is controlled by a growing static length scale ξ that is determined by the free energy landscape but not by the local dynamic rules governing its exploration. We argue, based on recent simulations using particle-radius-swap dynamics, that only a modest factor in the increase in τα on approach to the glass transition may stem from the growth of a static length, with a vastly larger contribution attributable, instead, to a slowdown of local dynamics. This reinforces arguments that we base on the observed strong coupling of particle diffusion and density fluctuations in real glasses.