Simulation of the Frequency Response of a Mach-Zehnder Modulator Actuated by a PZT Chip

Qiancheng Zhao1, Hao Lin1, Mingjian You1
1State Key Laboratory of Quantum Functional Materials, School of Microelectronics, Southern University of Science and Technology, Shenzhen, Guangdong 518000, China
Published in 2026

Integrating piezoelectric actuators onto photonic integrated circuits equips passive photonic components with active tunability and modulation capabilities [1]. Lead zirconate titanate (PZT) chips have been hybrid integrated onto microring resonators to demonstrate tunable external cavity lasers [2], as well as onto Mach-Zehnder interferometers to realize highly efficient phase modulation [3]. When electrically biased, the PZT chip induces mechanical deformation, which further introduces stress and strain to the underlying optical waveguide, altering its effective mode index via the stress-optic effect. While the modulation efficiency under static (DC) driving conditions has been numerically modeled [4] and been applied to control resonance splitting [5], systematic modeling of frequency response under alternating-current (AC) driving condition remains unexplored. In this work, we develop a 3D finite-element simulation model in COMSOL Multiphysics® to evaluate the electro-optic (EO) modulation bandwidth of a PZT-actuated photonic chip. Adopting the structural geometry from our prior experimental work [3], we establish a simplified 3D model comprising a top PZT actuator bonded to a SiO2/Ta2O5/SiO2 photonic platform. The PZT chip (TA0505D024W, Thorlabs®) is attached via a 150 μm-thick epoxy resin adhesive layer (EP31ND, Master Bond®), as shown in Fig. 1. Anisotropic piezoelectric and mechanical properties are assigned to each domain. We first perform a Stationary study with the help of the Solid Mechanics (solid) and Electrostatics (es) interfaces within the Structural Mechanics and AC/DC modules to analyze the static stress distribution on the photonic chip. Fig. 2 displays the structural deformation under a DC bias of 10 V. The induced in-plane stresses (Sx and Sy) along the cut-line [Fig. 3(a)] that passes through the waveguide layer is shown in Fig. 3(b). These results indicate that the transferred stress is highly spatially dependent, with the central region providing a relatively uniform biaxial stress in contrast to the sharp variations at the edges. To characterize the frequency response, we then conduct frequency domain study in the Structural Mechanics and AC/DC modules. A frequency sweep from 0 to 5000 Hz is performed at a fixed 10 V voltage amplitude. By evaluating the y-stress at the waveguide layer beneath the PZT center point, the frequency response is obtained in Fig. 4, revealing the 3 dB bandwidth is 2985 Hz. The simulated result aligns well with our experimental measurements. The EO bandwidth is primarily limited to the mechanical damping from the epoxy layer [2]. The simulation framework provides a robust design methodology for modeling and optimizing integrated Mach-Zehnder modulators and microring resonators that are actuated by top-bonded PZT chips.

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