We study facilitated models which extend to arbitrary dimensions the one-dimensional East process and which are supposed to catch some of the main features of the complex dynamics of fragile glasses. We focus on the low-temperature regime (small density c ≈ eβ of the facilitating sites). In the literature the relaxation process has been assumed to be quasione-dimensional and the equilibration time has been computed using the relaxation time of the East model (d = 1) on the equilibrium length scale Lc = (1/c)1/d in d-dimension. This led to a super-Arrhenius scaling for the relaxation time of the form Trel ?exp(β2/d log 2). In a companion paper, using renormalization group ideas and electrical networks methods, we rigorously establish that instead Trel exp(β2/2d log 2), contradicting the quasione-dimensional assumption. The above scaling confirms previous MCAMC simulations. Next we compute the relaxation time at finite and mesoscopic length scales, and show a dramatic dependence on the boundary conditions. Our final result is related to the out-of-equilibrium dynamics. Starting with a single facilitating site at the origin we show that, up to length scales L = O(L c), its influence propagates much faster (on a logarithmic scale) along the diagonal direction than along the axes directions. © 2014 EPLA.

The influence of dimension on the relaxation process of East-like models: Rigorous results / P., Chleboun; Faggionato, Alessandra; F., Martinelli. - In: EUROPHYSICS LETTERS. - ISSN 0295-5075. - STAMPA. - 107:3(2014), pp. 36002-36002-p6. [10.1209/0295-5075/107/36002]

The influence of dimension on the relaxation process of East-like models: Rigorous results

FAGGIONATO, ALESSANDRA;
2014

Abstract

We study facilitated models which extend to arbitrary dimensions the one-dimensional East process and which are supposed to catch some of the main features of the complex dynamics of fragile glasses. We focus on the low-temperature regime (small density c ≈ eβ of the facilitating sites). In the literature the relaxation process has been assumed to be quasione-dimensional and the equilibration time has been computed using the relaxation time of the East model (d = 1) on the equilibrium length scale Lc = (1/c)1/d in d-dimension. This led to a super-Arrhenius scaling for the relaxation time of the form Trel ?exp(β2/d log 2). In a companion paper, using renormalization group ideas and electrical networks methods, we rigorously establish that instead Trel exp(β2/2d log 2), contradicting the quasione-dimensional assumption. The above scaling confirms previous MCAMC simulations. Next we compute the relaxation time at finite and mesoscopic length scales, and show a dramatic dependence on the boundary conditions. Our final result is related to the out-of-equilibrium dynamics. Starting with a single facilitating site at the origin we show that, up to length scales L = O(L c), its influence propagates much faster (on a logarithmic scale) along the diagonal direction than along the axes directions. © 2014 EPLA.
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Utilizza questo identificativo per citare o creare un link a questo documento: http://hdl.handle.net/11573/645056
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