Arnaud Lazarus
Sorbonne Université, Paris, France
Seminar Information
A broad class of mechanical and physical systems is governed by linear differential equations with coefficients that vary periodically in time or space. Such periodic modulation gives rise to spectral lock-in regions that govern the system’s response. These lock-in regimes arise, for example, as parametric instabilities in dynamical systems and as band gaps in waves propagating through periodic media. Despite their ubiquity, these spectral mechanisms remain largely unexplored and unexploited in mechanical engineering.
In the first part of this talk, I will introduce the concept of spectral lock-in at the heart of the stability analysis of Floquet systems. I will show how it can be exploited to enhance parametric instabilities and to enrich buckling patterns in elastic structures subjected to periodically varying compressive stresses. In the second part, I will present a class of systems with periodic coefficients that exhibit discrete spectra directly analogous to those of the stationary Schrödinger equation. I will demonstrate how these ideas can be leveraged to design new quantum-inspired functionalities in engineering systems, including the dynamical stabilization of mechanical oscillators and the control of wave propagation in periodic media.
Arnaud Lazarus received a PhD degree in mechanical engineering from Ecole Polytechnique, Palaiseau, France, in 2008. After two post-doctoral years in Paris, he joined the Massachusetts Institute of Technology as an associate postdoctoral researcher from 2010 to 2013. In 2013, he became an associate professor at Sorbonne Université, Paris, France, doing his research at Institut Jean le Rond ∂’Alembert. In 2024, after a one-year sabbatical in Katia Bertoldi’s group within the School of Engineering and Applied Sciences at Harvard he joined the department of Mathematics at MIT, hosted by John W. Bush as an invited associate professor. His current interests include the stability of dynamical systems and the mechanics of slender elastic structures with a particular interest in Floquet-Bloch theory.