Non-Fermi Liquid Behavior in a Disordered Kondo Alloy Model

Physics – Condensed Matter – Strongly Correlated Electrons

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22 pages, 8 figures. Minor changes. References added. Accepted by Phys. Rev. B

Scientific paper

10.1103/PhysRevB.60.4702

We study a mean-field model of a Kondo alloy using numerical techniques and analytic approximations. In this model, randomly distributed magnetic impurities interact with a band of conduction electrons and have a residual RKKY coupling of strength $J$. This system has a quantum critical point at $J=J_{c} \sim T_{K}^0$, the Kondo scale of the problem. The $T$ dependence of the spin susceptibility near the quantum critical point is singular with $\chi(0)-\chi(T) \propto T^{\gamma}$ and non-integer $\gamma$. At $J_{c}$, $\gamma = 3/4$. For $J\lesssim J_{c}$ there are two crossovers with decreasing $T$, first to $\gamma=3/2$ and then to $\gamma=2$, the Fermi-liquid value. The dissipative part of the time-dependent susceptibility $\chi''(\omega)\propto \omega$ as $\omega \to 0$ except at the quantum critical point where we find $\chi''(\omega) \propto \sqrt{\omega}$. The characteristic spin-fluctuation energy vanishes at the quantum critical point with $\omega_{\rm sf} \sim (1-J/J_{c})$ for $J\lesssim J_{c}$, and $\omega_{\rm sf} \propto T^{3/2}$ at the critical coupling.

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