Abstract

Using time-dependent density matrix renormalization group calculations we study the transport properties ($I-V$ curves and shot noise) of the interacting resonant level model (IRLM) in a large range of the interaction parameter $U$, in the scaling limit. We find that these properties can be described remarkably well by those of the Boundary sine-Gordon model (BSG), which are known analytically (Fendley, Ludwig and Saleur, 1995). We argue that the two models are nevertheless in different universality classes out of equilibrium: this requires a delicate discussion of their infra-red (IR) properties ({\it i.e.} at low voltage), where we prove in particular that the effective tunneling charge is $e$ in the infra-red regime of the IRLM (except at the self-dual point where it jumps to $2e$), while it is known to be a continuously varying function of $U$ in the BSG. This behavior is confirmed by careful analysis of the numerical data in the IR. The remarkable agreement of the transport properties, especially in the crossover region, remains however unexplained.

Highlights

  • The field of out-of-equilibrium quantum many body systems has developed rapidly in the last decade

  • We find that these properties can be described remarkably well by those of the Boundary sine-Gordon model (BSG), which are known analytically (Fendley, Ludwig and Saleur, 1995)

  • We argue that the two models are in different universality classes out of equilibrium: this requires a delicate discussion of their infra-red (IR) properties, where we prove in particular that the effective tunneling charge is e in the infra-red regime of the interacting resonant level model (IRLM), while it is known to be a continuously varying function of U in the BSG

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Summary

INTRODUCTION

The field of out-of-equilibrium quantum many body systems has developed rapidly in the last decade. One of the very pleasant features of the BSG model is that it involves a freely adjustable parameter, which can be interpreted as the anomalous dimension of the tunneling operator at the UV or IR limit of the renormalization group flow, and characterizes, among others, the anomalous power laws in the I − V characteristics This parameter takes a fixed value in a given realization e.g. for a given value of the Luttinger liquid interaction, or the quantum Hall filling fraction. We show in particular, using bosonization and integrability in equilibrium, that the quasiparticles which tunnel across the dot have an effective charge e in the IR limit of the IRLM (except at the self-dual point, where it is 2e), which departs from the continuously varying charge in the BSG model This is confirmed by some numerical calculations of the backscattered current and shot noise at low bias in the IRLM at intermediate value of the interaction. Why the results for the IRLM and the BSG model are so close remains an open question, which we discuss some more in the conclusion

Hamiltonian
Quench protocols
Current
Charge fluctuations and shot noise
The BSG template
CURRENT
Comparison with the I-V curve of the BSG model
Large bias and cIRLM
Finite bias
CHARGE FLUCTUATIONS AND CURRENT NOISE
IRLM VERSUS BSG
The field-theoretic description
IR physics
Small bias and backscattered current
Charge of the carriers
SUMMARY AND CONCLUSIONS
Full Text
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