A spectroscopic technique for high-sensitivity gas sensing

A quartz-enhanced photo-acoustic gas sensor employing a custom quartz tuning fork enables extension of the technology into the terahertz range.
23 January 2014
Vincenzo Spagnolo, Pietro Patimisco, Angelo Sampaolo, Gaetano Scamarcio, Simone Borri, Harvey E. Beere, David A. Ritchie and Miriam S. Vitiello

Recent technological innovation in photonics and nanotechnology is stimulating the use of terahertz (THz) spectroscopic sensing systems in a wide variety of applications, including global environmental monitoring and homeland security. The THz region of the electromagnetic spectrum, however, remains largely unexplored. This is due to limited options for optical components, detectors, and tunable and powerful coherent sources.

Among the most robust and sensitive trace-gas detection techniques, quartz-enhanced photo-acoustic spectroscopy (QEPAS) is capable of record sensitivities in the mid-IR spectral range, with a compact and relatively low cost acoustic detection module.1 All QEPAS sensors reported thus far, however, exploit standard quartz-crystal tuning forks (QTFs), which have a resonance frequency of ∼32.76kHz and are characterized by a very small sensitive volume between their prongs (approximately 0.3×0.3×3mm3).2 Due to this small area, focusing the THz beam has represented the main limitation preventing the use of these QEPAS systems in the THz range (λ>50μm). Larger QTFs are therefore required for this purpose.

To focus the THz beam between the two prongs of the QTF without illuminating them, we employed a tuning fork with standard geometry, scaled to ∼6 times the size of a standard fork (see Figure 1). The custom QTF shows a quality factor in vacuum of Q0=146, 350 and a resonance frequency of f0=4245Hz, ∼8 times lower than that of standard QTFs.3, 4

Figure 1. Schematic of the employed custom quartz crystal tuning-fork (QTF) resonator. This QTF enables the focusing of a terahertz (THz) beam due to the larger area between its prongs (∼6 times the size of a standard tuning fork).

A schematic of our gas sensor QEPAS setup is shown in Figure 2. The laser source emits at 3.93THz, in resonance with a rotational-translational transition (change in energy level) of methanol with line strength S=4.28·10−21cm/mol. QEPAS is based on the photoacoustic effect (the conversion of light to sound in absorbing materials). Methanol, an important gas species, is useful for this purpose because the THz laser used is resonant with one of its main absorption levels. We used off-axis paraboloidal gold reflectors to focus the THz beam between the prongs of the tuning fork, which acts as an optoacoustic transducer. The 3D laser beam profile, measured using a pyroelectric camera, has a beam waist diameter of ∼430μm. This value falls well below the gap between the QTF prongs (∼800μm), allowing the beam to pass through without making contact.4

Figure 2. Schematic of the quartz-enhanced photo-acoustic spectroscopy trace gas sensor setup. 2f and 3f represent the lock-in measuring the second and third harmonic, respectively, of the related input signal. QCL: Quantum cascade laser.

We performed the QEPAS experiments by applying a sinusoidal modulation to the quantum cascade laser (QCL) current at the QTF resonance frequency (f0), while detecting the QTF response at the same frequency using a lock-in amplifier. QEPAS spectral measurements were performed by slowly scanning the laser wavelength over ∼0.025cm−1. To obtain optical frequency modulation of up to 0.01cm−1, we added the sinusoidal dither at f0 to the low-frequency voltage ramp using a power combiner. QEPAS measurements in locked mode were performed by keeping the laser wavelength fixed on the absorption peak frequency and modulating its current at f0.

To test the sensor, gas mixtures with different methanol concentrations were obtained by diluting methanol vapors—collected from a reservoir at the corresponding vapor pressure (∼120Torr at 300K)—with pressurized N2. For measurements at low concentrations, we used a certified 100 parts per million (ppm) methanol/N2 gas mixture. The results confirm that the QEPAS signal is proportional to the methanol concentration across the entire investigated concentration range, from 6.5% down to 100ppm.

To determine the best achievable sensitivity of the QEPAS sensor, we performed an Allan variance analysis, measuring and averaging the QEPAS signal in locked mode.3 For a four second averaging time, we extracted a minimum detection sensitivity of 7ppm. This corresponds to a normalized noise equivalent absorption of 2·10−10cm−1W/Hz½, comparable with the best result obtained by mid-IR QEPAS systems. Since the energy of the incident laser light is very low (few milli-electron volts), rotational levels are primarily involved in THz absorption processes. Rotational-translational relaxation rates were found to be up to three orders of magnitude faster with respect to vibrational-translational relaxation. The QEPAS signal is strongly dependent on these energy relaxation rates because the gas requires enough time to dissipate all absorbed laser power before a new pulse arrives. The possibility of working with fast relaxing transition levels allows the device to operate at low pressure, thereby gaining high QTF Q-factors (several tens of thousands), increasing the selectivity and sensitivity of the QEPAS sensor system.

In summary, we have outlined the first demonstration of a QEPAS sensor employing a THz QCL source and a custom QTF. The geometry of the QTFs employed thus far in QEPAS systems has been optimized only in terms of resonance frequency, i.e., for timing applications. The next step will therefore be the fabrication of QTFs with improved geometry to increase sensing performance and detection levels.

V. Spagnolo acknowledges financial support from the Italian national projects PON01_2238, PON02_0675, and PON02_0576.

Vincenzo Spagnolo
Physics Department
Polytechnic University of Bari
Institute of Photonics and Nanotechnology (IFN-CNR)
Bari, Italy

Vincenzo Spagnolo received his degree and PhD in physics from the University of Bari and currently works as assistant professor of physics. His research interests include QCLs and optoacoustic gas sensors.

Pietro Patimisco, Angelo Sampaolo, Gaetano Scamarcio
Physics Department
University of Bari
Bari, Italy
Simone Borri
National Institute of Optics (INO-CNR)
Bari, Italy
Harvey E. Beere, David A. Ritchie
Cavendish Laboratory
University of Cambridge
Cambridge, United Kingdom
Miriam S. Vitiello
NEST - Institute of Nanoscience (NANO-CNR)
Pisa, Italy

1. A. Elia, P. M. Lugarà, C. Di Franco, V. Spagnolo, Photoacoustic techniques for trace gas sensing based on semiconductor laser sources, Sensors 9(12), p. 9616-9628, 2009.
2. A. A. Kosterev, F. K. Tittel, D. V. Serebryakov, A. L. Malinovsky, I. V. Morozov, Applications of quartz tuning forks in spectroscopic gas sensing, Rev. Sci. Instrum. 76, p. 043105, 2005.
3. S. Borri, P. Patimisco, A. Sampaolo, H. E. Beere, D. A. Ritchie, M. S. Vitiello, G. Scamarcio, V. Spagnolo, Terahertz quartz enhanced photo-acoustic sensor, Appl. Phys. Lett. 103, p. 021105, 2013.
4. P. Patimisco, S. Borri, A. Sampaolo, H. E. Beere, D. A. Ritchie, M. S. Vitiello, G. Scamarcio, V. Spagnolo, A quartz enhanced photo-acoustic gas sensor based on custom tuning fork and terahertz quantum cascade laser, Analyst, 2013. First published online: 4 October. doi:10.1039/C3AN01219K
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