Mid-infrared ethene detection using difference frequency generation in a quasi-phase-matched LiNbO3 waveguide.

A periodically poled LiNbO3 (PPLN) crystal waveguide has been used to produce up to 200 microW of mid-infrared light around 3081 cm(-1) with a wide tunability range of approximately 35 cm(-1). Two commercial near-infrared diode lasers at 1.064 microm (pump) and 1.583 microm (signal) are mixed in a nonlinear optical crystal to achieve difference frequency generation. The 48 mm long directly-bonded quasi-phase-matched (QPM) PPLN waveguide shows a conversion efficiency of 12.3% W(-1). Applications in trace gas detection have been demonstrated for ethene, using multipass absorption coupled with wavelength modulation spectroscopy, and cavity enhanced absorption spectroscopy with a lock-in detection scheme: bandwidth reduced sensitivities of alpha(min)=8 x 10(-9) and 1.6 x 10(-8) cm(-1) Hz(-1/2)(2sigma), respectively, have been achieved.

[1]  L. Hollberg,et al.  Difference-frequency generation in PPLN at 4.25 μm: an analysis of sensitivity limits for DFG spectrometers , 2000 .

[2]  J. Burie,et al.  Continuous-wave mid-infrared laser sources based on difference frequency generation , 2007 .

[3]  Gang Li,et al.  The HITRAN 2008 molecular spectroscopic database , 2005 .

[4]  Z. Gong,et al.  Widely phase-matched tunable difference-frequency generation in periodically poled LiNbO3 crystal , 2008 .

[5]  Takeshi Umeki,et al.  Widely tunable 2.3 μm-band difference frequency generation in quasiphase-matched LiNbO3 ridge waveguide using index dispersion control , 2007 .

[6]  G. Hancock,et al.  Mid-infrared generation and spectroscopy with a PPLN ridge waveguide , 2007 .

[7]  Hiroyuki Suzuki,et al.  Wavelength Conversion Using Quasi-Phase Matched LiNbO3 Waveguides , 2005, IEICE Trans. Electron..

[8]  Andrey B. Krysa,et al.  λ∼3.1 μm room temperature InGaAs/AlAsSb/InP quantum cascade lasers , 2009 .

[9]  M. Fejer,et al.  Quasi-phase-matched optical parametric oscillators in bulk periodically poled LiNbO 3 , 1995 .

[10]  J. Giovannoni Genetic Regulation of Fruit Development and Ripening , 2004, The Plant Cell Online.

[11]  M. Sigrist,et al.  Near-infrared laser based cavity ringdown spectroscopy for applications in petrochemical industry , 2006 .

[12]  Combining preconcentration of air samples with cavity ring-down spectroscopy for detection of trace volatile organic compounds in the atmosphere. , 2004, Analytical chemistry.

[13]  Grant A. D. Ritchie,et al.  4 Cavity ring-down and cavity enhanced spectroscopy using diode lasers , 2005 .

[14]  Martin M. Fejer,et al.  Quasi-phasematched optical parametric oscillators using bulk periodically poled LiNbO3 , 1995, Photonics West.

[15]  K. Magari,et al.  Efficient 3-μm difference frequency generation using direct-bonded quasi-phase-matched LiNbO3 ridge waveguides , 2006 .

[16]  V. Aneja,et al.  Characterization of non-methane hydrocarbons in the rural southeast United States , 1997 .

[17]  J G Anderson,et al.  Ultrasensitive absorption spectroscopy with a high-finesse optical cavity and off-axis alignment. , 2001, Applied optics.

[18]  P. Hering,et al.  Online monitoring of ethane traces in exhaled breath with a difference frequency generation spectrometer , 2006 .

[19]  T. Walther,et al.  Application of a difference-frequency-mixing based diode-laser sensor for carbon monoxide detection in the 4.4–4.8 μm spectral region , 2006 .

[20]  D. Jundt,et al.  Temperature-dependent Sellmeier equation for the index of refraction, n(e), in congruent lithium niobate. , 1997, Optics letters.

[21]  P. De Natale,et al.  A 3.5-mW continuous-wave difference-frequency source around 3 μm for sub-Doppler molecular spectroscopy , 2005, EQEC '05. European Quantum Electronics Conference, 2005..

[22]  J. Henningsen,et al.  Quantitative wavelength-modulation spectroscopy without certified gas mixtures , 2000 .

[23]  Richard G. Derwent,et al.  Analysis and interpretation of the continuous hourly monitoring data for 26 C2–C8 hydrocarbons at 12 United Kingdom sites during 1996 , 2000 .

[24]  David H. Parker,et al.  Photoacoustic trace gas detection of ethene released by UV-induced lipid peroxidation in humans , 2000, European Conference on Biomedical Optics.

[25]  A. Parkes,et al.  Absorption cross-sections and pressure broadening of rotational lines in the v5 + v9 band of ethene measured by diode laser cavity ring down spectroscopy , 2004 .

[26]  Johannes Orphal,et al.  A continuous-wave difference-frequency generation laser operating in the mid-infrared (3-5 μm) region for accurate line intensity measurements , 2008 .

[27]  Grant A. D. Ritchie,et al.  Difference frequency generation in periodically poled lithium niobate and its use in the detection of atmospheric methane , 2004 .

[28]  Takeshi Umeki,et al.  Diode-laser based 3mW DFG at 3.4 /spl mu/m from wavelength conversion module using direct-bonded QPM-LN ridge waveguide , 2006 .

[29]  Yueming Qiu,et al.  Distributed Feedback Mid-IR Interband Cascade Lasers at Thermoelectric Cooler Temperatures , 2007, IEEE Journal of Selected Topics in Quantum Electronics.

[30]  R. Peverall,et al.  3.5-μm high-resolution gas sensing employing a LiNbO3 QPM-DFG waveguide module , 2009 .

[31]  G. Berden,et al.  Cavity ring-down spectroscopy: Experimental schemes and applications , 2000 .

[32]  Z. Gong,et al.  A difference frequency generation spectrometer and its detection of atmospheric N2O. , 2007, Spectrochimica acta. Part A, Molecular and biomolecular spectroscopy.