Abstract

High precision surface processing has an unmet demand for picosecond pulses with arbitrary temporal profiles in radial polarization states and at high average powers. Here, simultaneous spatial and arbitrary temporal shaping of chirped 10 - 100 picoseconds pulses is demonstrated with an Yb-doped fiber laser system generating an output power of more than 10 W at 40 MHz repetition frequency. The closed-loop control algorithm carves the pulses using a commercial, rugged, and fiberized optical pulse shaper placed at the front end of the system and uses feedback from the output pulse shapes for optimization. Arbitrary complex temporal profiles were demonstrated using a dispersive Fourier transform based technique and limits set by the system were investigated. Pulse shaping in the spatial domain was accomplished using an S-waveplate, fabricated in-house, to change the linearly polarized fundamental mode into a doughnut mode with radial polarization. This was amplified in a final-stage few-mode large-mode area fiber amplifier. Placing both temporal and spatial shaping elements before the power-amplifier avoids complex and potentially lossy conversion of the spatial mode profile at the output and provides an efficient route for power-scaling. The use of properly oriented quarter- and half-wave plates, which have both low loss and high power handling capability, enabled the output to be set to pure radial or azimuthal polarization states. Using commercial off-the-shelf components, our technique is able to immediately enhance the versatility of ultrashort fiber laser systems for high precision material processing and other industrial applications.

Highlights

  • High energy short pulse lasers are widely used for material processing in research laboratories [1, 2], as well as in industrial and military applications [3, 4]

  • We created a selection of temporal pulse profiles: square pulse, step pulse, double peak energy bridge (DPEB) and triple peak energy bridge (TPEB)

  • The gain in the final amplifier is ~20 dB but the ripples on the shaped spectrum that are often seen to arise with the onset of nonlinear effects in chirped-pulse amplification (CPA) systems are still within 2 dB

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Summary

Introduction

High energy short pulse lasers are widely used for material processing in research laboratories [1, 2], as well as in industrial and military applications [3, 4]. Master oscillator power amplifier (MOPA) source configurations provide several key advantages. These include the ability to accurately modulate the system at low power levels at the seed stage prior to substantial amplification, power scalability, and stable operation even at high power levels [5]. In order to pave the way to both improved and new material processing applications, researchers are exploring the use of different pulse shapes [6]. To optimize the processing of materials by type, or even of individual samples with different physical, chemical and mechanical properties, the pulse energy and the pulse shape in the time domain needs to be precisely controlled

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