Harnessing $\mathcal{P}\mathcal{T}$-symmetry in non-Hermitian stiffness-modulated waveguides

Abstract

The recent progress in the context of elastic metamaterials and modulated waveguides with digitally controllable properties has opened new pathways to overcome the limitations dictated by Hermitian Hamiltonians in mechanics. Among the possible implementations, non-Hermitian, $\mathcal{P}\mathcal{T}$-symmetric systems with balanced gain and loss have emerged as an elegant mechanism to access novel functionalities by lifting the non-Hermitian degeneracies (exceptional points). Motivated by this, the paper deals with a non-Hermitian and $\mathcal{P}\mathcal{T}$-symmetric elastic waveguide with complex stiffness-modulation. The strength of the stiffness-modulations, tailored in the form of a balanced gain/loss, delineates a transition from unbroken to broken $\mathcal{P}\mathcal{T}$-symmetric phases, where distinct Bloch-wave modes coalesce into exceptional points. It is shown that, in the unbroken $\mathcal{P}\mathcal{T}$-symmetric regime, and due to the interplay between real and imaginary components of the elasticity, the waveguide operates as a phononic filter. When the strength of the gain/loss interactions increases, the frequency gap closes and the bulk bands degenerate into an exceptional point, where the system operates as a waveguide with asymmetric scattering capabilities. The paper provides a connection between the distinct wave modes that populate the non-Hermitian degeneracies and the directional reflection/transmission capabilities. The asymmetric behavior is herein explained by combining the dispersion properties of a $\mathcal{P}\mathcal{T}$-symmetric rod, obtained through the plane wave expansion method (PWEM), and the scattering matrix method (SMM) for a modulated slab series-connected to semi-infinite media.

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Cited by in corpus (2)

• Complex Spatiotemporal Modulations and Non-Hermitian Degeneracies in $\mathcal{P}\mathcal{T}$-Symmetric Phononic Materials
• Non-Local Elastic Lattices with $\mathcal{P}\mathcal{T}$-Symmetry and Time Modulation: From Perfect Trapping to the Wave Boomerang Effect