# Resistivity minimum emerges in Anderson impurity model modified with   Sachdev-Ye-Kitaev interaction

**Authors:** Lan Zhang, Yin Zhong, Hong-Gang Luo

arXiv: 1905.03425 · 2019-05-10

## TL;DR

This paper studies a modified Anderson model with Sachdev-Ye-Kitaev interactions, revealing a resistivity minimum associated with a non-Fermi liquid state, distinct from traditional Kondo physics, and identifies a crossover from Fermi liquid to non-Fermi liquid behavior.

## Contribution

It introduces a novel Anderson model variant with SYK interactions, demonstrating a resistivity minimum linked to non-Fermi liquid behavior without Kondo resonance.

## Key findings

- Resistivity exhibits a minimum around a characteristic temperature.
- System transitions from Fermi liquid to non-Fermi liquid and then to a Fermi gas with temperature.
- Non-Fermi liquid behavior occurs without Kondo resonance in the density of states.

## Abstract

We investigate a modified Anderson model at the large-$N$ limit, where Coulomb interaction is replaced by Sachdev-Ye-Kitaev random interaction. The resistivity of conduction electron $\rho_{c}$ has a minimum value around temperature $\widetilde{T}_{K}$, which is similar to the Kondo system, but the impurity electron's density of state $A_{d}(\omega)$ elucidates no sharp-peak like Kondo resonance around the Fermi surface. The impurity electron's entropy $S_{d}$ and specific heat capacity $C_{\textrm{v}}$ illustrate a crossover from Fermi liquid to the non-Fermi liquid. The system is a non-Fermi liquid at temperature $T^{\star}<T<\widetilde{T}_{K}$, a Fermi liquid for $T<T^{\star}$, and becomes a Fermi gas if $T>\widetilde{T}_{K}$. The non-Fermi liquid at intermediate-$T$ regime does not occur in standard Anderson model. With renormalization group analysis, we elucidate a crossover from Fermi liquid to the non-Fermi liquid, coinciding with transport and thermodynamics. The resistivity minimum and the Kondo resonance are two characteristics of Kondo effect. However, the resistivity minimum emerges in our model when the system behaves as a NFL rather than FL, and the impurity electron's density of state without the Kondo resonance.

## Full text

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## Figures

17 figures with captions in the complete paper: https://tomesphere.com/paper/1905.03425/full.md

## References

57 references — full list in the complete paper: https://tomesphere.com/paper/1905.03425/full.md

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Source: https://tomesphere.com/paper/1905.03425