We report the temperature dependence of resistivity (ρ) and Hall coefficient (RH) in the normal state of homogeneously disordered epitaxial NbN thin films with kFl~1.68--10.12. The superconducting transition temperature (Tc) of these films varies from 2.7 to 16.8 K. While our least disordered film displays usual metallic behavior, for all the films with kFl≤8.13, both dρdT and dRHdT are negative up to 285 K. We observe thatRH(T) varies linearly with ρ(T) for all the films and $[{{R}H(T){-}{R}H(285 K)}{{R}H(285 K)}]={γ}[{{ρ}(T){-}{ρ}(285 K)}{{ρ}(285 K)}]$, where ${γ}=0.68±{}0.11$. Measurements performed on a 2-nm-thick Be film show similar behavior with ${γ}=0.69$. This behavior is inconsistent with existing theories of localization and $e{{-}}e$ interactions in a disordered metal.
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Chand et al. (2009) studied this question.
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