Abstract

We analyze ultrafast tunneling experiments in which electron transport through a localized orbital is induced by a single cycle THz pulse. We include both electron-electron and electron-phonon interactions on the localized orbital using the Anderson-Holstein model and consider two possible filling factors, the singly occupied Kondo regime and the doubly occupied regime relevant to recent experiments with a pentacene molecule. Our analysis is based on variational non-Gaussian states and provides the accurate description of the degrees of freedom at very different energies, from the high microscopic energy scales to the Kondo temperature $T_K$. To establish the validity of the new method we apply this formalism to study the Anderson model in the Kondo regime in the absence of coupling to phonons. We demonstrate that it correctly reproduces key properties of the model, including the screening of the impurity spin, formation of the resonance at the Fermi energy, and a linear conductance of $2e^2/h$. We discuss the suppression of the Kondo resonance by the electron-phonon interaction on the impurity site. When analyzing THz STM experiments we compute the time dependence of the key physical quantities, including current, the number of electrons on the localized orbital, and the number of excited phonons. We find long-lived oscillations of the phonon that persist long after the end of the pulse. We compare the results for the interacting system to the non-interacting resonant level model.

Highlights

  • Motivated by recent experiments in this paper we provide a theoretical analysis of THz-scanning tunneling microscopes (STM) experiments of tunneling through a single localized orbital, such as a highest occupied molecular orbital (HOMO) orbital in a pentacene molecule used by Cocker et al [7]

  • We demonstrate that our approach accurately captures the formation of the Kondo resonance at the Fermi energy with the width set by the Kondo energy scale

  • An appealing aspect of this method is that degrees of freedom at very different energy scales, from the local repulsion U to the Kondo temperature TK, are described within the same framework and without the numerical demands of the numerical renormalization group (NRG) and density matrix renormalization group (DMRG) calcualtions

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Summary

Motivation

Ultrafast experiments constitute a new approach to exploring quantum many-body systems and provide a platform for developing new types of solid-state devices for nanotechnology and quantum information processing (for review, see Refs. [1,2,3,4]). This technique allows to combine atomic spatial resolution of STM with subpicosecond coherent temporal control of electron currents Such experiments pose a new challenge to many-body theory to develop methods for analyzing the farout-of-equilibrium quantum dynamics of interacting manybody systems. We present a theoretical approach for analyzing nonequilibrium dynamics of the Anderson-Holstein impurity model. This method is based on the variational non-Gaussian wave functions introduced in Ref. Our second goal in this paper is to analyze a specific type of nonequilibrium dynamics: THz-STM experiments through a single molecule For such experiments we compute the time dependence of the key observables: current through the system, number of electrons on the molecule, and number of excited phonons. We discuss the difference in the results between the noninteracting RLM system and the Anderson-Holstein model

Anderson-Holstein model
Review of the theoretical formalism
Organization of the paper
Electron-phonon polaron transformation
Parity operator and impurity decoupling transformation
Gaussian part of the wave function
GROUND-STATE PROPERTIES
Equations of motion in imaginary time
Physical observables
Anderson model in equilibrium
REAL-TIME DYNAMICS
Equations of motion
Transport in the Anderson model
Transport in the Anderson-Holstein model
Discussion of results
SUMMARY AND OUTLOOK

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