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Slow Relaxation Near the Glass Transition: from the Tanaka model to glycerol Itamar Procaccia The Institute of Theoretical Physics The Chinese University of Hong Kong Work with: E. Lerner, T.S. Lo, V. Ilyin, H.G.E. Hentschel, I. Regev CUHK Sept 2008 Itamar Procaccia The Institute of Theoretical Physics The Chinese University of Hong Kong Work with: E. Lerner, T.S. Lo, V. Ilyin, H.G.E. Hentschel, I. Regev CUHK Sept 2008
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The Shintani-Tanaka model: One component liquid with anisotropic potential
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For the system crystallizes into hexagonal lattice with disordered ‘spins’. (The ground state has anti-ferromagnetic order). For the system fails to crystallize. Relaxation times were measured via the ‘spin’ autocorrelation function The results were fitted (as is customary in the field) to a stretched exponential form and the relaxation time was fitted to the Folger-Fulcher form Locally favoured structure
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In the interesting range of temperatures 0<T<0.5 one observes 36 different stars with In more than 98% of the n-stars the central particle has the ‘good’ angle with respect to two of its neigbors.
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Combinatorics The first factorial is the number of ways to choose the ‘good’ edges of the central particle This leaves I+j+k-2 edges to choose the red edges from There are 2-k green edges, and i red edges, and thus i-k+2 spins in ‘bad’ orientations. Therefore i+j+k-(I-k+2) ‘good’ ones.
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The constraint Total number of ‘green’ and ‘blue’ interactions in the system:
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The partition function AFM crystal
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The decrease of a concentration to zero introduces a natural length-scale
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Modeling the relaxation functions
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The physics of the slowing down
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Broad-band dielectric spectroscopy
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Imagine clusters of correlated molecules in a bath of ‘liquid’.
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The relaxation time The distribution of cluster sizes
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The Gibbs free energy The chemical potential of the smallest cluster Constraint (very important !!)
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Changing surface energy
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Experiments in pores
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The riddle of the data collapse
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