We study the interplay of electron-electron and electron-disorder scattering in correlated Fermi liquids by the disordered Hubbard model using dynamical mean-field theory with an IPT-CPA solver. We find significant violations of Matthiessen’s rule (additivity of scattering mechanisms) that we explain in terms of the screening of the disorder potential by interactions, leading to a protection of the electron-electron inelastic scattering rate against disorder. We also show that large disorder can lead to a surprising enhancement of the electron-electron scattering that contrasts with the competition seen in the elastic channel. Our results compare positively with available resistivity data in the disordered Fermi liquid phase of the correlated organic metals $\kappa \text{−}{(\mathrm{ET})}_2\mathrm{X}$, and rationalize the strong sample dependence of the $T^2$ coefficients observed in the resistivity of correlated perovskite oxides such as ${\mathrm{SrVO}}_3$.

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• Electrical conductivity
• Transport phenomena
• Strongly correlated systems
• Dynamical mean field theory