Inverse Freezing in Mean-Field Models of Fragile Glasses
arXiv:cond-mat/0603381 · doi:10.1103/PhysRevB.73.180202
Abstract
A disordered spin model suitable for studying inverse freezing in fragile glass-forming systems is introduced. The model is a microscopic realization of the ``random-first order'' scenario in which the glass transition can be either continuous or discontinuous in thermodynamic sense. The phase diagram exhibits a first-order transition line between two fluid phases terminating at a critical point. When the interacting degrees of freedom are entropically favoured an inverse static glass transition and a double inverse dynamic freezing appear.
arXiv comment4 pages, 4 figures
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