Abstract
The statistical mechanics of vulcanized (i.e. permanently randomly crosslinked) macromolecular matter can be formulated, using the replica technique, as the n to 0 limit of a theory containing n+1 coupled replicas. Within the framework of a replica-symmetric variational mean-field approach, this theory describes an equilibrium phase transition, upon sufficient vulcanization, from a liquid to an amorphous solid state. We consider a natural extension of this framework, which admits the possibility of the spontaneous breaking of replica symmetry, and find that-at least at the mean-field level-replica symmetry appears to remain intact. We discuss the physical origin of this absence of replica-symmetry breaking, as well as a possible strategy for a theoretical refinement that may yield replica-symmetry breaking.
| Original language | English |
|---|---|
| Article number | 011 |
| Pages (from-to) | 6375-6381 |
| Number of pages | 7 |
| Journal | Journal of Physics A: Mathematical and General |
| Volume | 27 |
| Issue number | 19 |
| DOIs | |
| State | Published - 1994 |
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