The singular response in the thermodynamic and geometric properties of manifolds pinned by quenched disorder to local and global perturbations is considered. The averaged displacement of a linear-extent L manifold is proportional to pLₚ^ζ+φ, where p is the (small pLₚ^-1/φ) magnitude of the perturbation, {ζ} is the unperturbed roughness exponent, and φₚ is a crossover exponent which is calculated for a variety of uniform and random perturbations. Applications to random magnets, polymers, flux lines, and magnetoresistance of localized electrons are discussed.
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Yonathan Shapir (1991) studied this question.
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