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We study the effects of localization on the Hall transport in a granular
system at large tunneling conductance corresponding to the
metallic regime. We show that the first-order in 1/g_T weak localization
correction to Hall resistivity of a two- or three-dimensional granular array
vanishes identically, . This result is in agreement with
the one for ordinary disordered metals. Being due to an exact cancellation, our
result holds for arbitrary relevant values of temperature T and magnetic field
H, both in the homogeneous'' regime of very low T and H corresponding to ordinary disordered metals and in the structure-dependent’’ regime of higher
values of T or H.

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