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Higher order interaction effects have been examined in two- and three-dimensional weakly localized regime for the case of Coulomb interactions. The quantum corrections of the conductivity and the magnetoresistance are determined to the linear order of \(λ = /2 π ε Fτ \), ε F and τ being the Fermi energy and the life time, respectively, but to the infinite order in the interaction strength, F .
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Isawa et al. (1984) studied this question.
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