Abstract

This paper presents a KGW Raman laser with an external-cavity configuration in the 2 μm region. The Raman laser is pumped by unique, electro-optic, actively Q-switched Tm:Yap laser, emitting at 1935 nm. The electro-optic modulation is based on a KLTN crystal, enabling the use of a short crystal length, with a relatively low driving voltage. Due to the KGW bi-axial properties, the Raman laser is able to lase separately at two different output wavelengths, 2273 and 2344 nm. The output energies and pulse durations for these two lines are 0.42 mJ/pulse at 18.2 ns, and 0.416 mJ/pulse at 14.7 ns, respectively. This is the first implementation of a KGW crystal pumped by an electro-optic active Q-switched Tm:Yap laser in the SWIR spectral range.

Highlights

  • Lasers emitting at 2–3 μm enhance a wide variety of applications because of their relatively high absorption coefficients and the interesting atmospheric window at this spectral range

  • Raman lasers leverage the principles of stimulated Raman scattering (SRS) to shift the light that comes into the crystal by a frequency corresponding to the vibrational frequency of the material

  • In 2018 we reported the first Raman laser in the 2 μm region based on a KGW crystal

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Summary

Introduction

Lasers emitting at 2–3 μm enhance a wide variety of applications because of their relatively high absorption coefficients and the interesting atmospheric window at this spectral range. They are used in LIDAR; microsurgery [1]; the processing of polymers, semiconductors, and metals [2]; defense applications; and gas sensing industries [3]. Pumping Raman cavities at very high peak power densities enables frequency conversion and produces new laser lines and useful high-brightness sources. This extends the spectral spans of existing lasers and fills the spectral gaps in this spectral range [4,5,6,7]. Raman lasers have a few more advantages, such as linewidth narrowing, pulse length shortening, and spatial beam quality improvement through Raman beam cleanup [8]

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