Abstract

The century-old study of photon–phonon coupling has seen a remarkable revival in the past decade. Driven by early observations of dynamical back-action, the field progressed to ground-state cooling and the counting of individual phonons. A recent branch investigates the potential of traveling-wave, optically broadband photon–phonon interaction in silicon circuits. Here, we report continuous-wave Brillouin gain exceeding the optical losses in a series of suspended silicon beams, a step towards selective on-chip amplifiers. We obtain efficiencies up to the highest to date in the phononic gigahertz range. We also find indications that geometric disorder poses a significant challenge towards nanoscale phonon-based technologies.

Highlights

  • The interaction between photons and acoustic phonons has been investigated in bulk materials since the 1920s [1, 2]

  • In case the phonons are generated by optical forces, the interaction is often called stimulated Brillouin scattering (SBS) – a feedback loop in which energy flows from the optical waves to the mechanical oscillator

  • Through a novel opto-acoustic nanodevice, a series of suspended silicon wires, we demonstrate modest (0.5 dB) net Brillouin gain with high efficiencies

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Summary

Introduction

The interaction between photons and acoustic phonons has been investigated in bulk materials since the 1920s [1, 2]. The removal of the bandwidth restriction and the accompanying optical versatility has motivated a great deal of SBS work in small-core waveguides, from photonic crystal [6,7,8], dual-web [9] and subwavelength [10] fibres to chalcogenide [11,12,13] and silicon waveguides [14,15,16]. Mass-manufacturable siliconon-insulator chips are an exciting platform for high-density optomechanical circuitry, perhaps even at the quantum level [19,20,21] Recent work on this front has demonstrated promising photon-phonon coupling efficiencies in all-silicon waveguides [16]. From a wider perspective and not limited to our system, such geometric disorder may hinder development of nanoscale phonon circuits quite generally [19,20,21, 23]

Theoretical background
TPA and tan φ
Optomechanical experiments
Conclusion
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