Motivated by the intrinsic non-Fermi-liquid behavior observed in the heavy-fermion quasicrystal Au₅₁Al₃₄Yb₁₅, we study the low-temperature behavior of dilute magnetic impurities placed in metallic quasicrystals. We find that a large fraction of the magnetic moments are not quenched down to very low temperatures T, leading to a power-law distribution of Kondo temperatures P(TK)~TK^α-1, with a nonuniversal exponent α, in a remarkable similarity to the Kondo-disorder scenario found in disordered heavy-fermion metals. For α<1, the resulting singular P(TK) induces non-Fermi-liquid behavior with diverging thermodynamic responses as T→0.
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Andrade et al. (2015) studied this question.
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