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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.

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Presentation on theme: "Slow Relaxation Near the Glass Transition: from the Tanaka model to glycerol Itamar Procaccia The Institute of Theoretical Physics The Chinese University."— Presentation transcript:

1 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

2 The Shintani-Tanaka model: One component liquid with anisotropic potential

3 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

4 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.

5 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.

6 The constraint Total number of ‘green’ and ‘blue’ interactions in the system:

7 The partition function AFM crystal

8 The decrease of a concentration to zero introduces a natural length-scale

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10 Modeling the relaxation functions

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12 The physics of the slowing down

13 Broad-band dielectric spectroscopy

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15 Imagine clusters of correlated molecules in a bath of ‘liquid’.

16 The relaxation time The distribution of cluster sizes

17 The Gibbs free energy The chemical potential of the smallest cluster Constraint (very important !!)

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20 Changing surface energy

21 Experiments in pores

22 The riddle of the data collapse

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