Abstract

Non-Fermi liquids are strange metals whose physical properties deviate qualitatively from those of conventional metals due to strong quantum fluctuations. In this paper, we report transport measurements on the FeSe$_{1-x}$S$_x$ superconductor, which has a quantum critical point of a nematic order without accompanying antiferromagnetism. We find that in addition to a linear-in-temperature resistivity $\rho_{xx}\propto T$, which is close to the Planckian limit, the Hall angle varies as $\cot \theta_{\rm H} \propto T^2$ and the low-field magnetoresistance is well scaled as $\Delta\rho_{xx}/\rho_{xx}\propto \tan^2 \theta_{\rm H}$ in the vicinity of the nematic quantum critical point. This set of anomalous charge transport properties shows striking resemblance with those reported in cuprate, iron-pnictide and heavy fermion superconductors, demonstrating that the critical fluctuations of a nematic order with ${\bf q} \approx 0$ can also lead to a breakdown of the Fermi liquid description.

Highlights

  • One of the most prominent features in many strongly correlated superconductors is that critical antiferromagnetic (AFM) fluctuations emanating from an AFM quantum critical point (QCP) seriously modify the quasiparticle masses and scattering cross section of the Fermi liquid, leading to non-Fermi liquid (NFL) behaviors [1,2]

  • We find that in addition to a linear-in-temperature resistivity ρxx ∝ T, which is close to the Planckian limit, the Hall angle varies as cot θH ∝ T 2 and the low-field magnetoresistance is well scaled as ρxx/ρxx ∝ tan2 θH in the vicinity of the nematic quantum critical point

  • We demonstrate anomalous low-field transport properties in FeSe1−xSx superconductor, which has a QCP of an electronic nematic order that is not accompanied by sizable magnetic fluctuations

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Summary

Introduction

One of the most prominent features in many strongly correlated superconductors is that critical antiferromagnetic (AFM) fluctuations emanating from an AFM quantum critical point (QCP) seriously modify the quasiparticle masses and scattering cross section of the Fermi liquid, leading to non-Fermi liquid (NFL) behaviors [1,2]. In these systems, the highest superconducting transition temperature Tc is often observed near the QCP. The resistivity at low temperatures is often dominated by inelastic electron-electron scattering. The resistivity from this mechanism varies as ρxx ∝ T 2, which is taken as an experimental

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