Electroacoustic Metamaterials

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Picture of the Active Metacrystal platform developped by Mathieu Padlewski. Credit: Alain Herzog@EPFL

Introduction

From the Greek ÎŒÎ”Ï„ÎŹ – meta, meaning “beyond”, acoustic metamaterials are artificially structured materials designed to exhibit extraordinary acoustic properties not typically found in nature – such as negative bulk modulus (K), negative mass density (ρ), and even negative refractive index (n). These remarkable properties allow sound to be controlled in ways that conventional materials cannot achieve.

However, traditional (passive) acoustic metamaterials are inherently limited: their behaviour is decided and fixed during the design and fabrication, they often operate only over narrow frequency bands, and they experience significant losses due to resonator-based mechanisms. Because of this, their use is restricted in practical applications like acoustic prisms, carpet cloaks and leaky-wave antenna (see photo gallery below).

Active electroacoustic metamaterials overcome these limitations. By combining acoustic elements with electronic control they can manipulate sound waves in real time. Unlike passive systems, which rely solely on geometry and material properties, active metamaterials integrate sensors, actuators, and digital controllers to dynamically tune their response (similarly to the Active Electroacoustic Resonator concept). This enables advanced wave phenomena such as nonreciprocity, topological insulation, and amplitude-driven confinement, offering promise for a new generation of adaptive and high-performance acoustic devices.

How it works

Based on the Active Electroacoustic Resonator concept, each unit cell typically includes a microphone to sense incoming pressure waves, a controller (DSP or FPGA) to compute the desired response, and loudspeaker diaphragm to exert a controlled force. The microphone picks up local sound pressure, the controller calculates the required diaphragm force to shape the local acoustic impedance, and the amplifier drives the diaphragm to absorb, reflect or reroute sound waves as needed.

When arrayed, these components form a feedback loop that allows the metamaterial to behave as a programmable medium. By adjusting parameters like impedance, coupling strength, and nonlinearity, researchers can simulate complex physical models that go beyond the natural realm. 

What are the applications

Active electroacoustic metamaterials have broad and impactful applications, especially in room acoustics and noise control engineering. These include noise control through adaptive cancellation and absorption in changing environments; architectural acoustics with real-time tuning of reverberation and reflections; acoustic imaging via beam steering and resolution enhancement; topological acoustics enabling robust sound transport immune to defects; nonreciprocal devices that allow one-way sound transmission for communication and sensing; and energy localisation through amplitude-driven confinement for energy harvesting and wave trapping.

What we are working on

Our recent research focuses on nonlocal and nonlinear coupling between resonators, enabling the study of exotic forms of matter. This includes amplitude-driven topological transitions, demonstrating that increasing the driving amplitude can switch the system between different topological regimes (learn more about amplitude-driven topological confinement of sound, active acoustic Su-Schrieffer-Heeger-Like metamaterials and chiral linearity for topological protection). We also explore non-Hermitian and nonlinear wave manipulation, investigating the interplay of nonlocality, nonlinearity, and non-Hermiticity in classical wave systems (learn more about amplitude-driven nonreciprocity for energy guiding). Additionally, we study cochlear mechanisms, as the cochlea is composed of an array of active hair cells which can be modelled by our system (learn more here).

These innovations are validated through a fully programmable experimental platform capable of dynamically reconfiguring the acoustic response of the system.

 

List of projects associated with this topic

Funding body Project Period
SNSF Active Nonlinear AcousticMETAsurfaces 2021-2025

To learn more

2025

Experimental assessment of a programmable Electroacoustic Liner in a representative turbofan facility

E. De Bono; E. Salze; M. Collet; M. Gillet; M. Ouisse et al. 

Applied Acoustics. 2025. Vol. 240, num. 5, p. 110896. DOI : https://doi.org/10.1016/j.apacoust.2025.110896.

Active control of electroacoustic resonators in the audible regime: control strategies and airborne applications

M. MallĂ©jac; M. Volery; H. Lissek; R. Fleury 

npj Acoustics. 2025. Vol. 1, num. 1. DOI : 10.1038/s44384-025-00006-9.

Observation of amplitude-driven nonreciprocity for energy guiding

M. F. Padlewski; R. Fleury; H. Lissek 

Physical Review B. 2025. Vol. 111, num. 12. DOI : 10.1103/PhysRevB.111.125156.

2023

Active Acoustic Su-Schrieffer-Heeger-Like Metamaterial

M. F. Padlewski; M. Volery; R. Fleury; H. Lissek; X. Guo 

Physical Review Applied. 2023. Vol. 20, p. 014022. DOI : 10.1103/PhysRevApplied.20.014022.

Ultrabroadband sound control with deep-subwavelength plasmacoustic metalayers

S. Sergeev; R. Fleury; H. Lissek 

Nature Communications. 2023. num. 14, p. 2874. DOI : 10.1038/s41467-023-38522-5.

Observation of non-reciprocal harmonic conversion in real sounds

X. Guo; H. Lissek; R. Fleury 

Communications Physics. 2023. Vol. 6, num. 93, p. 1 – 6. DOI : 10.1038/s42005-023-01217-w.

2020

Improving sound absorption through nonlinear active electroacoustic resonators

X. Guo; R. Fleury; H. Lissek 

Physical Review Applied. 2020. Vol. 13, p. 014018. DOI : 10.1103/PhysRevApplied.13.014018.

2019

Active acoustic resonators with reconfigurable resonance frequency, absorption, and bandwidth

T. Koutserimpas; E. Rivet; H. Lissek; R. Fleury 

Physical Review Applied. 2019. Vol. 12, num. 5, p. 054064. DOI : 10.1103/PhysRevApplied.12.054064.

Acoustic rat-race coupler and its applications in non-reciprocal systems

F. Zangeneh Nejad; R. Fleury 

The Journal of the Acoustical Society of America. 2019. Vol. 146, num. 1, p. 843 – 849. DOI : 10.1121/1.5115020.

2018

Constant-pressure sound waves in non-Hermitian disordered media

E. Rivet; A. Brandstötter; K. G. Makris; H. Lissek; S. Rotter et al. 

Nature Physics. 2018. Vol. 14, p. 942 – 947. DOI : 10.1038/s41567-018-0188-7.

Toward Wideband Steerable Acoustic Metasurfaces with Arrays of Active Electroacoustic Resonators

H. Lissek; E. Rivet; T. Laurence; R. Fleury 

Journal of Applied Physics. 2018. Vol. 123, num. 9, p. 091714. DOI : 10.1063/1.5011380.

2017

Generation of acoustic helical wavefronts using metasurfaces

H. Esfahlani; H. Lissek; J. R. Mosig 

Physical Review B. 2017. Vol. 95, num. 2, p. 024312. DOI : 10.1103/PhysRevB.95.024312.

2016

Acoustic dispersive prism

H. Esfahlani; S. Karkar; H. Lissek; J. R. Mosig 

Scientific Reports. 2016. Vol. 6, p. 18911. DOI : 10.1038/srep18911.

Acoustic carpet cloak based on an ultrathin metasurface

H. Esfahlani; S. Karkar; H. Lissek; J. R. Mosig 

Physical Review B. 2016. Vol. 94, num. 1, p. 014302. DOI : 10.1103/PhysRevB.94.014302.

Exploiting the leaky-wave properties of transmission-line metamaterials for single-microphone direction finding

H. Esfahlani; S. Karkar; H. Lissek; J. R. Mosig 

The Journal of the Acoustical Society of America. 2016. Vol. 139, num. 6, p. 3259 – 3266. DOI : 10.1121/1.4949544.

2010

Acoustic transmission line metamaterial with negative/zero/positive refractive index

F. Bongard; H. Lissek; J. R. Mosig 

Physical Review B. 2010. Vol. 82, num. 9, p. 094306. DOI : 10.1103/PhysRevB.82.094306.