I. Introduction
Ultrasound is widely used in biomedical and industrial manufacturing, such as cardiac ultrasound, endovascular endoscopy, abdominal ultrasound, and gynecological ultrasound due to its high sensitivity, noninvasiveness, low cost, and high resolution [1]–[7]. The high resolution and sensitivity of the ultrasonic transducer will result in high-quality imaging [8], [9]. Sensitivity is reduced due to the large attenuation of high-frequency sound waves, which affects the penetration distance. The lateral resolution is limited by the diameter of piezo-element and center frequency. However, the lateral resolution can be significantly improved by applying an external lens or mechanical ball pressure, whereas the axial resolution is directly determined by the performance (bandwidth and center frequency) of the ultrasonic transducers [10], [11]. A large bandwidth tends to form narrow pulses, which will greatly improve the axial resolution [12]–[14]. Therefore, excellent performance (high frequency, large bandwidth, and high sensitivity) is the goal that researchers in ultrasonic imaging have been pursuing. In particular, how to obtain wide bandwidth ultrasonic transducers by effective methods has always been a great challenge [15]–[17].