The collective dynamics of particles in random energies and with a narrow distributed random coordination number shows a dynamical transition. The characteristic macroscopic time scale averaged over the coordination number and the energy distribution diverges with an essential singularity, i.e. as the celebrated Vogel-Fulcher law which is widely used in the treatment of experimental data for the viscosity and relaxation times of glass forming liquids.
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Thomas A. Vilgis (1990) studied this question.