Abstract

Laser ultrasound offers several benefits in comparison to immersion or air-coupled ultrasound: it directly generates stress on the sample surface; it has a wide bandwidth and a small acoustic source can be produced. Conventionally, high-power pulsed lasers are required therefore equipment is bulky and expensive. Here we propose to use mid-power laser diodes, which are small and low cost. To solve the low signal amplitude problem with lower power lasers, the use of spread spectrum signal, arbitrary position, and width binary pulse sets is proposed. To date, a laser driver for this task has not been available. This article describes the development of such a compact driver, where the essential electronics occupy an area of $10\,\,\times20$ mm. The whole system with a fixture for kinematic mount is comparable in size to a conventional piezoelectric ultrasonic transducer. The driver can supply pulse sets of up to 40 A. Individual pulse duration can vary between 20 and 1000 ns (0.5–25-MHz ultrasound range) and the total pulse train duration is limited by the laser type used. Experiments show that up to 10- $\mu \text{s}$ long pulse sets can be used at 10-A current, without laser degradation. Current waveforms, beam profile, and optical response signals were measured for three rectified topologies. It was concluded that the GaN-based constant current switch topology has the best performance, but a power MOSFET in a source current feedback topology can also be used to generate pulses down to 20 ns. Photoacoustic response signals from chirp and phase shift keying modulation have been demonstrated.

Highlights

  • UULTRASONIC measurement and imaging are used widely across a range of application areas

  • Noncontact transduction is possible using air-coupled ultrasound which can be challenging with high impedance mismatches, or electromagnetic acoustic transducers (EMATs) which whilst being non-contact still must be within a few millimetres of the sample surface [5]-[7]

  • The current loop inductance reduction was achieved from the printed circuit board (PCB) layout

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Summary

INTRODUCTION

UULTRASONIC measurement and imaging are used widely across a range of application areas. Laser ablation can change the material surface, so subsequent signals are different if obtained in the same location [9] and material damage occurs, where coating or surface layers with different properties to the bulk are removed by the first laser beam shot Another problem, related to the thermoelastic regime laser ultrasound is the production of dual acoustic pulse when the free surface thermoelastic source is used. There are applications that make use of the angled or surface waves [14],[31]-[35], and others that require the main beam to be directed normal to the surface In these cases a constrained (buried) laser ultrasound source can be considered (sometimes addressed as fourth regime in laser ultrasound). The experimental investigation of the ultrasound generation on an acoustic delay line is presented, demonstrating that the spectral content of the ultrasonic signal can be controlled using the APWP sequences, described in [69] and [73]

Attainable Power Density
APWP Sequence Parameters
LASER DRIVER DEVELOPMENT
Main Switch FET
FET Driver
Parasitics
Driver Topologies Analysis
Current Sensing
Optical System
EXPERIMENTAL INVESTIGATION RESULTS
Boosted MOSFET Source Current Feedback Laser Driver
GaN Boosted Resistor Current Limiter Laser Driver
GaN Constant Current Sink Laser Driver
Beam Profile
Acoustic Output
CONCLUSION
Full Text
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