Sound Wave Manipulation Based on Valley Acoustic Interferometers

TL;DR

This paper introduces topological valley acoustic interferometers using Y-shaped sonic crystals, demonstrating tunable sound manipulation through interference and Berry phase effects, with potential for advanced acoustic device design.

Contribution

It presents a novel design of topological valley acoustic interferometers with experimental validation and a new method for measuring interface dispersion efficiently.

Findings

Successful tuning of acoustic energy partition rate.

Verification of erry phase accumulation.

Enhanced measurement method for interface dispersion.

Abstract

Topological acoustics provides new opportunities for materials with unprecedented functions. In this work, we report a design of topological valley acoustic interferometers by Y-shaped valley sonic crystals. By tight-bounding calculation and experimental demonstration, we successfully tune the acoustic energy partition rate by configuring the channel. An analytical theory proposed to explain the transmission property matches well with experimental observations. An additional {\pi} Berry phase is verified to accumulate circling along the shape-independent topological valley acoustic interferometer, unique in the pseudospin half systems. Based on the spectral oscillation originating from the accumulated dynamic phase and {\pi} Berry phase, a simplified method to measure acoustic valley interface dispersion is explored, which overcomes the shortcomings of the traditional fast Fourier transform method and improves the measuring efficiency by simply analyzing the peaks and dips of the measured transmission spectrum. Moreover, an effective approach to tuning its transmissions, as well as the spectral line shapes proposed and realized by the local geometry design of the interferometer, exhibits strong tunability under an unchanged physical mechanism. Our work opens an avenue to design future acoustic devices with the function of sound wave manipulation based on the physical mechanism of interference and Berry phase.