I. Introduction
Seismic physical model (SPM), as a scaled analog to geological structures, has become a successful tool for research of seismic wave propagation [1]–[3]. At present, one of the key issues in SPM technique is the effective detection of sound fields. It relies on the availability of highly sensitive ultrasound sensors in order to be suitable for detection to the area of interest [4]. Ultrasonic waves (UWs) in SPM have normally weak amplitude, which requires a high-sensitivity sensor [5]. Piezoelectric transducers (PZTs) have been widely used for SPM detection. However, they suffer strongly resonant effects and offer lower sensitivities at smaller sizes [6], [7]. Comparatively, optical ultrasound detection offers several advantages, such as wider detection bandwidths, higher sensitivities at smaller sizes, and resistance to electromagnetic noise [8].