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Microscopic theory for the glass transition in a system without static correlations

2002/10/16 by R Schilling, Rolf Schilling, Grzegorz Szamel +1 · 2 citations
Chemistry · Materials Science · Physics and Astronomy · #Advanced Physical and Chemical Molecular Interactions #Material Dynamics and Properties #Theoretical and Computational Physics #cond-mat.soft #cond-mat.stat-mech

paper · pdf · doi:10.1209/epl/i2003-00214-6

6 pages, 3 figures

arxiv created 2002/10/16 · openalex publication_date 2003/01/01 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/04

Abstract

We study the orientational dynamics of infinitely thin hard rods of length L , with the centers-of-mass fixed on a simple cubic lattice with lattice constant a . We approximate the influence of the surrounding rods onto dynamics of a pair of rods by introducing an effective rotational diffusion constant D ( l ), l = L / a . We get D ( l ) ∝ [1 − υ( l )], where υ( l ) is given through an integral of a time-dependent torque-torque correlator of an isolated pair of rods. A glass transition occurs at l c , if υ( l c ) = 1. We present a variational and a numerically exact evaluation of υ( l ). Close to l c the diffusion constant decreases as D ( l ) ∝ ( l c − l ) γ , with γ = 1. Our approach predicts a glass transition in the absence of any static correlations, in contrast to the present form of mode-coupling theory.

Citations

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