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Recently, a new technology that can detect sub-wavelength surface cracks using Rayleigh wave generated by ultrasonic laser has been developed. In 2017, Ammar [22] studied the effect of ultrasonic laser frequency on the detection of sub-wavelength surface cracks using a new laser-based ultrasonic detection technology. Ultrasonic laser has a high resolution in comparison to the frequency of traditional ultrasonic transducers and the number of ultrasonic laser is small, so it is a good choice to detect the sub-wavelength surface cracks. In 2018, Tournat [23] investigated the influence of ultrasonic laser source on the distance to the crack tip and the angle to get the more effective Rayleigh waves for the detection of sub-wavelength surface cracks. In 2019, Ammar [24] studied the laser based ultrasonic detection technology to detect sub-wavelength surface cracks. Laser based ultrasonic wave generated by ultrasonic laser was used to detect sub-wavelength surface cracks and the results showed that the laser based detection can detect the sub-wavelength surface cracks without any influence of the propagation path in the environment while the ultrasonic laser is still transmitted to the crack tip. In 2020, Tournat [25] studied the rayleigh waves based ultrasonic detection technology to detect sub-wavelength surface cracks. And the results showed that the detection of sub-wavelength surface crack depends on the ultrasonic laser beam leading to a better signal-to-noise ratio.

In this work, the detection of sub-wavelength surface cracks is achieved using Rayleigh wave generation by an ultrasonic laser. The schematic diagram of the ultrasonic laser based Rayleigh wave generation technique and the experimental setup are shown in Fig. 1. The ultrasonic laser beam is focused into the specimen, and it impacts on the upper surface of the specimen to generate Rayleigh waves. The ultrasonic laser is generated by an optical fiber amplifier, a laser diode (LD) and a photodiode (PD). The laser beam from the LD passes through a laser diode driver (LDD) and is amplified by the optical fiber amplifier. Then the amplified laser beam is focused by an optical lens into the sample. Under the focal position, the laser beam is reflected by the upper surface of the sample. The reflected laser beam and the transmitted laser beam pass through the optical lens and PD. The PD converts the laser beam into current by photoelectric conversion.

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