Abstract

We discuss Kondo behavior of a conduction electron system coupled with local optical phonon by analyzing the Anderson-Holstein model with the use of a numerical renormalization group (NRG) method. There appear three typical regions due to the balance between Coulomb interaction UeeU_{\rm ee} and phonon-mediated attraction UphU_{\rm ph}. For Uee>UphU_{\rm ee}>U_{\rm ph}, we observe the standard Kondo effect concerning spin degree of freedom. Since the Coulomb interaction is effectively reduced as UeeUphU_{\rm ee}-U_{\rm ph}, the Kondo temperature TKT_{\rm K} is increased when UphU_{\rm ph} is increased. On the other hand, for Uee<UphU_{\rm ee}<U_{\rm ph}, there occurs the Kondo effect concerning charge degree of freedom, since vacant and double occupied states play roles of pseudo-spins. Note that in this case, TKT_{\rm K} is decreased with the increase of UphU_{\rm ph}. Namely, TKT_{\rm K} should be maximized for UeeUphU_{\rm ee} \approx U_{\rm ph}. Then, we analyze in detail the Kondo behavior at Uee=UphU_{\rm ee}=U_{\rm ph}, which is found to be explained by the polaron Anderson model with reduced hybridization of polaron and residual repulsive interaction among polarons. By comparing the NRG results of the polaron Anderson model with those of the original Anderson-Holstein model, we clarify the Kondo behavior in the competing region of UeeUphU_{\rm ee} \approx U_{\rm ph}.Comment: 8 pages, 8 figure

    Similar works

    Full text

    thumbnail-image

    Available Versions

    Last time updated on 03/01/2020