Abstract

We demonstrate mid-infrared dual-comb spectroscopy with an optical parametric oscillator (OPO) toward real-time field measurement. A singly resonant OPO based on a MgO-doped periodically poled lithium niobate (PPLN) crystal is demonstrated. Chirped mirrors are used to compensate the dispersion caused by the optical cavity and the crystal. A low threshold of 17 mW has been achieved. The OPO source generates a tunable idler frequency comb between 2.7 and 4.7 μm. Dual-comb spectroscopy is achieved by coupling two identical Yb-fiber mode-locked lasers to this OPO with slightly different repetition frequencies. A measured absorption spectrum of methane is presented with a spectral bandwidth of $$300\,\hbox {cm}^{-1}$$ , giving an instrumental resolution of $$0.4\,\hbox {cm}^{-1}$$ . In addition, a second OPO containing two MgO-doped PPLN crystals in a singly resonant ring cavity is demonstrated. As such, this OPO generates two idler combs (average power up to 220 mW), covering a wavelength range between 2.7 and 4.2 μm, from which a mid-infrared dual-comb Fourier transform spectrometer is constructed. By detecting the heterodyned signal between the two idler combs, broadband spectra of molecular gases can be observed over a spectral bandwidth of more than $$350\,\hbox {cm}^{-1}$$ . This special cavity design allows the spectral resolution to be improved to $$0.2\,\hbox {cm}^{-1}$$ without locking the OPO cavity, indicating that this OPO represents an ideal high-power broadband mid-infrared source for real-time gas sensing.

Highlights

  • Laser absorption spectroscopy plays an important role in a variety of applications including industrial processing control, biomedical research, frequency metrology, and environmental monitoring

  • Since its invention in the late 1990s, frequency combs have revolutionized optical frequency metrology [3], and provide new opportunities for other applications, especially for gas detection based on laser absorption spectroscopy [4]

  • A single optical frequency comb source can be treated as a coherent superposition of hundreds of thousands of CW lasers, and it is noted to be an ideal source for laser spectroscopy in terms of high spectral power, broad spectral bandwidth, high coherence, and frequency accuracy [5]

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Summary

Introduction

Laser absorption spectroscopy plays an important role in a variety of applications including industrial processing control, biomedical research, frequency metrology, and environmental monitoring. Wavelength modulation and frequency modulation spectroscopy based on continuous-wave (CW) lasers are typical techniques for sensitive trace gas detection with possible measurement time of 1 s. Within these approaches, only a small portion of the wavelength region can be covered, limiting these methods for real-time applications of multi-gas detection [2]. Since its invention in the late 1990s, frequency combs have revolutionized optical frequency metrology [3], and provide new opportunities for other applications, especially for gas detection based on laser absorption spectroscopy [4]. A single optical frequency comb source can be treated as a coherent superposition of hundreds of thousands of CW lasers, and it is noted to be an ideal source for laser spectroscopy in terms of high spectral power, broad spectral bandwidth, high coherence, and frequency accuracy [5]

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