The critical properties of systems with quenched bond disorder are determined from a fixed distribution, under renormalization group, of the random bonds. Full fixed distributions with all moments are obtained numerically by histograms and, to a good approximation, in terms of Γ distributions. For such systems, the specific-heat exponent α does not equal the crossover exponent φ at random criticality. We derive a new relation between α and φ, which invokes characteristics of the fixed distribution. The difference between α and φ is noted for n-vector models in 4-ε dimensions and for Potts models on hierarchical lattices solved exactly. In general, stable random critical behavior with positive α appears to be possible. We develop a general treatment of quenched disorder and illustrate it by calculating specific-heat curves. It is suggested that the critical exponents of the three- and four-state random-bond Potts models in two dimensions are ν1.06 and 1.19.
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Andelman et al. (1984) studied this question.
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