2021/06/12 by Mojahed, Alireza, Tsakmakidis, Kosmas L., Bergman, Lawrence A. +1
#Applied Physics (physics.app-ph) #FOS: Physical sciences #Materials Science (cond-mat.mtrl-sci) #Optics (physics.optics)
paper · doi:10.48550/arxiv.2106.06814
The classical 'time-bandwidth' limit for linear time-invariant (LTI) devices asserts that it is impossible to store broadband waves (large Δω's) for long times (large Δt's). For standing waves, i.e., vibrations, in particular, this limit takes on a simple form, Δt Δω = 1, where Δω is the bandwidth over which localization occurs, and Δt is the storage time. It remains a fundamental challenge in classical wave physics and vibration engineering to try to find ways to overcome this limit, not least because that would allow for storing broadband waves for long times, or achieve broadband resonance for low damping. Recent theoretical studies have suggested that such a feat might be possible in LTI terminated unidirectional waveguides or LTI topological 'rainbow trapping' devices, although an experimental confirmation of either concept is still lacking. In this work, we consider a nonlinear but time-invariant mechanical system and demonstrate experimentally that its time-bandwidth product can exceed the classical time-bandwidth limit, thus achieving values, both, above and below unity, in an energy-tunable way. Our proposed structure consists of a single degree-of-freedom nonlinear oscillator, rigidly coupled to a nondispersive waveguide. Upon developing the full theoretical framework for this class of nonlinear systems, we show how one may control the nonlinear flow of energy in the frequency domain, thereby managing to disproportionally decrease (increase) Δt, the storage time in the resonator, as compared with an increase (decrease) of the system's bandwidth Δω. Our results pave the way to conceiving and harnessing hitherto unattainable broadband and simultaneously low-loss wave-storage devices, both linear and nonlinear, for a host of key applications in wave physics and engineering.