Journal
PHYSICAL REVIEW APPLIED
Volume 18, Issue 4, Pages -Publisher
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevApplied.18.044013
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Funding
- US National Science Foundation
- University at Buffalo (SUNY) through the Buffalo Blue Sky Program
- [1847254]
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Unraveling real eigenfrequencies in non-Hermitian PT-symmetric Hamiltonians has opened new avenues in various fields. In this study, we investigate the wave propagation behavior of a one-dimensional non-Hermitian elastic medium with a universal complex stiffness modulation. We analyze the onset of complex conjugate eigenfrequencies and the existence conditions for wave-number gaps, and demonstrate the coalescence of multiple Bloch-wave modes at exceptional points.
Unraveling real eigenfrequencies in non-Hermitian PT-symmetric Hamiltonians has opened avenues in quantum physics, photonics, and most recently, phononics. However, the existing literature squarely focuses on exploiting such systems in the context of scattering profiles (i.e., transmission and reflection) at the boundaries of a modulated waveguide, rather than the rich dynamics of the non-Hermitian medium itself. In this work, we investigate the wave propagation behavior of a one-dimensional non-Hermitian elastic medium with a universal complex stiffness modulation that encompasses a static term in addition to real and imaginary harmonic variations in both space and time. Using a plane-wave expansion, we conduct a comprehensive dispersion analysis for a wide set of subscenarios to quantify the onset of complex conjugate eigenfrequencies, and set forth the existence conditions for gaps that emerge along the wave -number space. Upon defining the hierarchy and examining the asymmetry of these wave-number gaps, we show that both the position with respect to the wave-number axis and the imaginary component of the oscillatory frequency largely depend on the modulation type and gap order. Finally, we demonstrate the coalescence of multiple Bloch-wave modes at the emergent exceptional points where significant direction -dependent amplification can be realized by triggering specific harmonics through a process that is detailed herein.
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