Abstract
A general theory is given for the quenched dilute s-state Potts and n-vector models in any dimension d. It is shown that for T→0 at the percolation threshold the Potts thermal exponent νT equals the percolation exponent νp, implying a crossover exponent φ=1, for any s and d. For the n-vector model (n>1), νT=νp/ζR, where ζR is a resistivity critical exponent. Agreement with recent experiments for two-dimensional dilute Ising and Heisenberg systems is excellent.
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