Abstract

Tunable mid-infrared ultrashort lasers have become an essential tool in vibrational spectroscopy in recent years. They enabled and pushed a variety of spectroscopic applications due to their high brilliance, beam quality, low noise, and accessible wavelength range up to 20 µm. Many state-of-the-art devices apply difference frequency generation (DFG) to reach the mid-infrared spectral region. Here, birefringent phase-matching is typically employed, resulting in a significant crystal rotation during wavelength tuning. This causes a beam offset, which needs to be compensated to maintain stable beam pointing. This is crucial for any application. In this work, we present a DFG concept, which avoids crystal rotation and eliminates beam pointing variations over a broad wavelength range. It is based on two independently tunable input beams, provided by synchronously pumped parametric seeding units. We compare our concept to the more common DFG approach of mixing the signal and idler beams from a single optical parametric amplifier (OPA) or oscillator (OPO). In comparison, our concept enhances the photon efficiency of wavelengths exceeding 11 µm more than a factor of 10 and we still achieve milliwatts of output power up to 20 µm. This concept enhances DFG setups for beam-pointing-sensitive spectroscopic applications and can enable research at the border between the mid- and far-IR range due to its highly efficient performance.

Highlights

  • The application of ultrafast MIR lasers with high repetition rates for spectroscopy has enabled a variety of novel research topics, which have not been feasible before

  • In recent years, there have been a vast variety of new devices based on MIR optical parametric oscillators (OPOs) [11,12,13], intrapulse difference frequency generation (DFG) [14], DFG between the signal and idler beams of an near-infrared optical parametric amplifier (OPA) or OPO [9,15,16,17,18,19], or supercontinuum-seeded DFGs [20,21]

  • We conducted measurements using our dual OPO/OPA DFG setup, which offers an additional degree of freedom resulting from the decoupled input beams, compared to the signal-idler DFG setup

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Summary

Introduction

The application of ultrafast MIR lasers with high repetition rates for spectroscopy has enabled a variety of novel research topics, which have not been feasible before. The modern world is based on highly technical processes and their impact will further grow in search of solutions for renewable energy sources, environmentally friendly transportation, remote sensing, life sciences, or for the growing digitization. Research in these fields can significantly benefit from vibrational spectroscopy in the mid-infrared spectral region using ultrafast laser sources due to their excellent beam profile, high brilliance and power, low RMS and intensity noise and their excellent long-term stability [1,8,9,10]. To maintain the coupling into subsequent spectroscopic devices, this offset needs to be accurately compensated, requiring active electronic or time-consuming manual compensation or counter-rotating compensation optics, all of which impede the application of parametric MIR light sources

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