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
Summary
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
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