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For recent reviews, see (a) articles in the frontiers of material science in Science 267, 1615 (1995)
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Model glassy systems may be categorized into two classes. The first class includes models which have a trivial Hamiltonian. The glassy behavior in this class of models is due to kinetic constraints present in the models. Facilitated kinetic Ising models [G. H. Fredrickson and H. C. Andersen, Phys. Rev. Lett. 53, 1244 (1984)]
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for further discussions on the dynamics of this class of model systems. The second class of models are characterized by their nontrivial random or/and frustrated Hamiltonians, which give rise to glassy behavior. Potts glass, p-spin-interaction spin glass models
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See J. Jäckle, Prog. Theor. Phys. Suppl. 126, 53 (1997), for further discussions on the dynamics of this class of model systems. The second class of models are characterized by their nontrivial random or/and frustrated Hamiltonians, which give rise to glassy behavior. Potts glass, p-spin-interaction spin glass
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and the frustrated lattice gas model [M. Nicodemi and A. Coniglio, Phys. Rev. E 57, R39 (1998)], as well as the present model belong to this class. The nature of the possible relationship between these two classes is an important question to be resolved.
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