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We consider short-range classical spin glasses, or other disordered systems, consisting of Ising spins. For a low-temperature Gibbs state in infinite size in such a system, for given random bonds, it is controversial whether its decomposition into pure states will be trivial or non-trivial. We undertake a general study of the overall structure of this problem, based on metastates, which are essential to prove the existence of a thermodynamic limit. A metastate is a probability distribution on Gibbs states, for given disorder, that satisfies certain covariance properties. First, we prove that any metastate can be decomposed as a mixture of indecomposable metastates, and that all Gibbs states drawn from an indecomposable metastate are alike macroscopically. Next, we consider stochastic stability of a metastate under random perturbations of the disorder, and prove that any metastate is stochastically stable. Dynamically-frozen states play a role in the analysis of Gibbs states drawn from a metastate, either as states or as parts of states. Using a mapping into real Hilbert space, we prove results about Gibbs states, and classify them into six types. Any indecomposable metastate has a compact symmetry group, though it may be trivial; we call this a metasymmetry. Metastate-average states are studied, and can be related to states arising dynamically at long times after a quench from high temperature, under some conditions. Many features that are permitted by general results are already present in replica symmetry breaking (RSB). Our results are for cases both with and without spin-flip symmetry of the Hamiltonian and, technically, we use mixed p-spin--interaction models.
N. Read (Tue,) studied this question.