Abstract

Acousto-optic modulation (AOM) is regarded as an effective way to link multi-physical fields on-chip. We propose an on-chip AOM scheme based on the thin-film lithium niobate (TFLN) platform working at the higher-order TE1 mode, rather than the commonly used fundamental TE0 mode. Multi-physical field coupling analyses were carried out to obtain the refractive index change of the optical waveguide (>6.5×10−10 for a single phonon) induced by the enhanced acousto-optic interaction between the acoustic resonator mode and the multimode optical waveguide. By using a Mach-Zehnder interferometer (MZI) structure, the refractive index change is utilized to modulate the output spectrum of the MZI, thus achieving the AOM function. In the proposed AOM scheme, efficient mode conversion between the TE0 and TE1 mode is required in order to ensure that the AOM works at the higher-order TE1 mode in the MZI structure. Our results show that the half-wave-voltage-length product (VπL) is <0.01 V·cm, which is lower than that in some previous reports on AOM and electro-optic modulation (EOM) working at the fundamental TE0 mode (e.g., VπL > 0.04 V·cm for AOM, VπL > 1 V·cm for EOM). Finally, the proposed AOM has lower loss when compared with EOM because the electrode of the AOM can be placed far from the optical waveguide.

Highlights

  • Accepted: 23 December 2021Acousto-optic modulation (AOM) connecting the electric, mechanical, and optical fields, takes a vital role in the microwave, lightwave, and quantum photonic signal processing [1,2,3,4,5]

  • We find that the converted TE1 mode has a high mode purity and low mode crosstalk, contributing to the efficient operation of the AOM working at the higher-order TE1 mode

  • We have proposed an on-chip AOM based on the typical thin-film lithium niobate (TFLN) platform, in which the optical waveguide is a multimode waveguide supporting the higher-order

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Summary

Introduction

Acousto-optic modulation (AOM) connecting the electric, mechanical, and optical fields, takes a vital role in the microwave, lightwave, and quantum photonic signal processing [1,2,3,4,5]. Comparing with integrated electro-optic modulations (EOMs) [6,7,8,9,10], AOM typically works with multiple physical fields and its basic working process can be described as follows. The generated acoustic wave would interact with the optical mode of the waveguide, leading to a change in the mode effective index of the optical waveguide. The mode effective index change is used to modulate the output spectrum via waveguide structures, such as a Mach-Zehnder interferometer (MZI) [1,3] or microring resonator (MRR) [1,4]. On-chip integrated AOM can enhance the AOM performance and reduce the device dimension, but requires an ideal material platform to ensure efficient couplings between the different physical fields

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