Abstract

We study the time evolution and steady state of the charge current in a single-impurity Anderson model, using matrix product states techniques. A nonequilibrium situation is imposed by applying a bias voltage across one-dimensional tight-binding leads. Focusing on particle-hole symmetry, we extract current-voltage characteristics from universal low-bias up to high-bias regimes, where band effects start to play a dominant role. We discuss three quenches, which after strongly quench-dependent transients yield the same steady-state current. Among these quenches we identify those favorable for extracting steady-state observables. The period of short-time oscillations is shown to compare well to real-time renormalization group results for a simpler model of spinless fermions. We find indications that many-body effects play an important role at high-bias voltage and finite bandwidth of the metallic leads. The growth of entanglement entropy after a certain time scale (proportional to the inverse of Delta) is the major limiting factor for calculating the time evolution. We show that the magnitude of the steady-state current positively correlates with entanglement entropy. The role of high-energy states for the steady-state current is explored by considering a damping term in the time evolution.

Highlights

  • Over the past decade, experimental control over quantum systems has increased considerably

  • We studied the single-impurity Anderson model out of equilibrium beyond the linear response regime by means of density matrix renormalization group

  • We find that the period of characteristic oscillations in the time evolution of the charge current is already very well described by renormalization group results for a different model, the interacting resonant level model of spinless fermions

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Summary

INTRODUCTION

Experimental control over quantum systems has increased considerably. The steady state is obtained by combining density matrix renormalization group[7,11] (DMRG) and time evolving block decimation[9,11] (TEBD) techniques to perform real-time evolution of the system after several different quenches This technique is known to yield reliable results for a wide parameter range of one-dimensional models[12,13,14,24,25,26,27,28,29,30,31,32,33,34] and to agree with analytical data.[13]. We explain how we calculate the ground state using DMRG and the realtime evolution using TEBD

Single-impurity Anderson model
Quench preparation
Methods
TRANSIENT RESPONSE
Characteristic oscillations of the current
STEADY-STATE CURRENT
Extracting the steady-state current
Current-voltage characteristics
Comparison to previous results
Comparison to a noninteracting device
DISCUSSION
Time scales in the high-bias regime
ROLE OF HIGH-ENERGY STATES
CONCLUSIONS
Obtaining the current
Finite-size effects
Trotter error: δτ
MPS matrix dimension: χ
Comparison to analytical results

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