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VOLUME 57 (1993) | ISSUE 2 | PAGE 116
Conditions for the existence of a glass phase in disordered systems described by a weak-crystallization Hamiltonian of a general type
The behavior of disordered systems described by a generalized weak-crystallization Hamiltonian is examined. Systems of this sort contain a region with a phase of the spin-glass type. An expression is derived for the surface which bounds the region. This is a surface of third-order phase transitions. The free energy of the glass phase near the surface is calculated in the leading approximation.