Out-of-equilibrium impurities with correlated electrons: Spectral and transport properties

Text

Simple approximations to impurities with correlated electrons fail out of equilibrium, leading to an unphysical hysteresis loop in the current-voltage characteristics. Electron correlations are known to suppress this hysteresis. We applied a two-particle semianalytic approach to an out-of-equilibrium Anderson impurity attached to two biased metallic leads. The theory qualitatively correctly interpolates between weak and strong coupling. It is based on reduced parquet equations adapted to capture the critical regions of singularities in the Bethe-Salpeter equations. This advanced approach covers one-particle and two-particle thermodynamic and spectral quantities relatively well in both weak and strong coupling. Our approximation successfully suppressed the unphysical hysteresis loop. Furthermore, we qualitatively reproduced within the linear response the three transport regimes with the increasing temperature: from the Kondo resonant tunneling through the Coulomb-blockade regime up to a sequential tunneling regime. Far from equilibrium, we find that the bias plays a similar role as the temperature in destroying the Kondo resonant peak when the corresponding energy scale is comparable with the Kondo temperature. Aside from that, the applied voltage in low bias was shown to develop spectral peaks around the lead chemical potentials as observed in previous theoretical and experimental studies.

I-V characteristic curve of the Anderson impurity model.
Description
I-V characteristic curve of the Anderson impurity model at half-filling for interaction U = 40Γ and temperature T = 0.1Γ in the Coulomb-blockade regime calculated by the Hartree-Fock (HF) mean-field, GW approximation, and the reduced parquet equations (RPE). An unphysical hysteresis loop appears in the HF and GW approximations, with the solid line corresponding to the nonmagnetic solution and the dashed line to the magnetic one. The RPE suppresses the spurious magnetic order, hence it is free of hysteresis. Here, Γ is the energy unit, impurity bandwidth. The inset shows the magnetic susceptibility as a function of the bias voltage V.

Contact person: Václav Janiš