The field of disordered systems provides many simple models in which the competing influences of thermal and non-thermal disorder lead to new phases and non-trivial thermal behavior of order parameters. In this paper, we add a model to the subject by considering a system where the state space consists of various orderings of a list. As in spin glasses, the disorder of such "permutation glasses" arises from a parameter in the Hamiltonian being drawn from a distribution of possible values, thus allowing nominally "incorrect orderings" to have lower energies than "correct orderings" in the space of permutations. We analyze a Gaussian, uniform, and symmetric Bernoulli distribution of energy costs, and, by employing Jensen's inequality, derive a general condition requiring the permutation glass to always transition to the correctly ordered state at a temperature lower than that of the non-disordered system, provided that this correctly ordered state is accessible. We in turn find that in order for the correctly ordered state to be accessible, the probability that an incorrectly-ordered component is energetically favored must be less than the inverse of the number of components in the system. We show that all of these results are consistent with a replica symmetric ansatz of the system and argue that there is no permutation glass phase characterized by replica symmetry breaking, but there is glassy behavior represented by a residual entropy at zero temperature. We conclude by discussing an apparent duality between permutation glasses and fermion gases.

Relative to the previous version (and the journal paper), this version includes a necessary citation and provides a new phase diagram and interpretation of glassy behavior