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We consider interaction effects in a granular normal metal at not very low temperatures. Assuming that all weak localization effects are suppressed by the temperature we replace the initial Hamiltonian by a proper functional of phases and study the possibility for a phase transition depending on the tunneling conductance . It is demonstrated for any dimension that, while at small the conductivity decays with temperature exponentially, its temperature dependence is logarithmic at large The formulae obtained are compared with an existing experiment and a good agreement is found.

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