Abstract

Quantum interference is a striking manifestation of one of the basic concepts of quantum mechanics: the particle-wave duality. A spectacular visualization of this effect is the standing wave pattern produced by elastic scattering of surface electrons around defects, which corresponds to a modulation of the electronic local density of states and can be imaged using a scanning tunnelling microscope. To date, quantum-interference measurements were mainly interpreted in terms of interfering electrons or holes of the underlying band-structure description. Here, by imaging energy-dependent standing-wave patterns at noble metal surfaces, we reveal, in addition to the conventional surface-state band, the existence of an 'anomalous' energy band with a well-defined dispersion. Its origin is explained by the presence of a satellite in the structure of the many-body spectral function, which is related to the acoustic surface plasmon. Visualizing the corresponding charge oscillations provides thus direct access to many-body interactions at the atomic scale.

Highlights

  • Quantum interference is a striking manifestation of one of the basic concepts of quantum mechanics: the particle-wave duality

  • The invention of the scanning tunnelling microscope[2] (STM) allowed the visualization of this effect in the real space by looking at the spectacular standing wave patterns produced by elastic scattering of electrons and holes at surface defects, such as vacancies, adsorbates, impurities or step edges[3,4,5,6]

  • This finite lifetime results in a broadening of the peaks related to the local density of states8 (LDOS) oscillation wavevectors in Fourier transformed (FT) quasi-particle interference (QPI) maps[18]

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Summary

Introduction

Quantum interference is a striking manifestation of one of the basic concepts of quantum mechanics: the particle-wave duality. These waves, known as Friedel oscillations[7], correspond to modulations of the electronic local density of states[8] (LDOS) and can be energetically resolved by differential conductivity (dI/dU) maps, usually measured at low temperature to reach a large coherence length and an improved energy resolution.

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