Abstract: We investigate a modified Anderson model at the large-N limit, where the Coulomb interaction is replaced by the Sachdev-Ye-Kitaev random interaction. The resistivity of conduction electron ρ _c has a minimum value around temperature $T^\star$, which is similar to the Kondo system, but the impurity electron's density of state A _d(ω) demonstrates no sharp-peak like the Kondo resonance around the Fermi surface. This provides a counterintuitive example where resistivity minimum exists without Kondo resonance. The impurity electron's entropy S _d and specific heat capacity $C_v$ show a crossover from Fermi liquid to a non-Fermi liquid behavior dependent on temperature. The system is a Fermi liquid at $T<T^\star$ and becomes a non-Fermi liquid at $T>T^\star$, and then becomes a Fermi gas at sufficiently high temperatures $T\gg T^\star$. The non-Fermi liquid at the intermediate-T regime does not occur in the standard Anderson model. We also make a renormalization group analysis, which confirms the crossover from Fermi liquid to the non-Fermi behavior. It is emphasized that the resistivity minimum emerges in our model when the system behaves as a non-Fermi liquid rather than Fermi liquid, which provides an alternative example showing resistivity minimum in condensed matter physics.

Key words: Anderson model, Sachdev-Ye-Kitaev interaction, non-Fermi liquid