Optical-feedback cavity-enhanced absorption spectroscopy with an interband cascade laser: application to SO2 trace analysis

The combination of interband cascade lasers (ICL) with cavity-enhanced absorption spectroscopy (CEAS) offers new perspectives in trace analysis and isotope ratio measurements. ICLs cover a mid-infrared spectral window (3–4 µm), in between those covered by Ga(InAs)Sb diode lasers and quantum cascade lasers (QCL), where strong molecular transitions can be found. While ICLs have lower emission power than QCLs, their thermal dissipation is much closer to that of telecom diode lasers and their current tuning range larger, which are both major advantages for developing compact instruments. We present an OF-CEAS implementation with an ICL at 4.015 µm, in which optical feedback (OF) enables efficient injection into the high-finesse cavity. In this paper, we also discuss a procedure allowing to obtain an accurate measurement of the OF rate. With regard to performance, we obtain a rms noise-equivalent absorption of 7.7 × 10−9 cm−1 for one acquired spectrum (80 ms) with a cavity of finesse 3900, which translates to a normalized figure of merit of 2.2 × 10−9 cm−1/√Hz, allowing for SO2 trace analysis down to ppbv levels with a response time of seconds.

[1]  A. McGonigle,et al.  Total volatile flux from Mount Etna , 2008 .

[2]  Grant A. D. Ritchie,et al.  Optical feedback cavity-enhanced absorption spectroscopy with a 3.24 μm interband cascade laser , 2015 .

[3]  Peter Werle,et al.  Diode-Laser Sensors for In-Situ Gas Analysis , 2004 .

[4]  A. Clairon,et al.  Frequency noise analysis of optically self-locked diode lasers , 1989 .

[5]  B. Mizaikoff,et al.  Breath analysis with broadly tunable quantum cascade lasers. , 2013, Analytical chemistry.

[6]  Tao Liu,et al.  Ambient air pollution and years of life lost in Ningbo, China , 2016, Scientific Reports.

[7]  V. M. Devi,et al.  The 2009 edition of the GEISA spectroscopic database , 2011 .

[8]  Daniele Romanini,et al.  Cavity Enhanced Absorption Spectroscopy with Optical Feedback , 2014 .

[9]  P. Werle,et al.  The limits of signal averaging in atmospheric trace-gas monitoring by tunable diode-laser absorption spectroscopy (TDLAS) , 1993 .

[10]  Daniele Romanini,et al.  A water isotope (2H, 17O, and 18O) spectrometer based on optical feedback cavity-enhanced absorption for in situ airborne applications , 2006 .

[11]  M. Carras,et al.  Optical-feedback cavity-enhanced absorption spectroscopy with a quantum cascade laser. , 2010, Optics letters.

[12]  F. Dong,et al.  Photonic Sensing of the Atmosphere by absorption spectroscopy , 2012 .

[13]  D. Romanini Modelling the excitation field of an optical resonator , 2014 .

[14]  Clive Oppenheimer,et al.  Sulfur Degassing From Volcanoes: Source Conditions, Surveillance, Plume Chemistry and Earth System Impacts , 2011 .

[15]  H. Fischer,et al.  Quantum Cascade Laser Spectrometry Techniques: A New Trend in Atmospheric Chemistry , 2013 .

[16]  Daniele Romanini,et al.  Fast, low-noise, mode-by-mode, cavity-enhanced absorption spectroscopy by diode-laser self-locking , 2005 .

[17]  F. Tittel,et al.  Quartz-enhanced photoacoustic spectroscopy-based sensor system for sulfur dioxide detection using a CW DFB-QCL , 2014 .

[18]  M. Carras,et al.  Optical-feedback cavity-enhanced absorption spectroscopy with a quantum-cascade laser yields the lowest formaldehyde detection limit , 2013, Applied Physics B.

[19]  K. Shimaoka,et al.  Effect of aging on the concentrations of nitrous oxide in exhaled air. , 1997, The Science of the total environment.