Journal of Spectroscopy
Volume 2015 (2015), Article ID 218413, 6 pages
http://dx.doi.org/10.1155/2015/218413

Research Article

Multi-Quartz Enhanced Photoacoustic Spectroscopy with Different Acoustic Microresonator Configurations

Huadan Zheng,1,2 Xukun Yin,1,2 Lei Dong,1,2 Hongpeng Wu,1,2 Xiaoli Liu,1,2 Weiguang Ma,1,2 Lei Zhang,1,2 Wangbao Yin,1,2 and Suotang Jia1,2

¹State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser Spectroscopy, Shanxi University, Taiyuan 030006, China
²Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China

Received 16 September 2015; Accepted 22 October 2015

Academic Editor: Arnaud Cuisset

Copyright © 2015 Huadan Zheng et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

Acoustic microresonators were added to the recently developed multi-QTF based QEPAS spectrophone to enhance the signal amplitude. Two kinds of “on-beam” configurations were experimentally investigated in detail. The developed multi-QTF based “on-beam” spectrophone had a signal enhancement of 1.6 times compared with the traditional single QTF based “on-beam” spectrophone, with the approximate noise level. A normalized noise equivalent absorption coefficient () of 1.24 × 10⁻⁹ W·cm⁻¹·Hz−1/2 was obtained for water vapor detection at atmospheric pressure.

1. Introduction

Laser absorption spectroscopy for trace gas detection has gained considerable interest over the past decades. Among optical spectroscopic techniques, photoacoustic spectroscopy (PAS) is a well-established sensitive approach, with the advantages of zero-background nature, excitation-wavelength independence, and linear dependence of signal amplitudes on excitation powers [1–4]. As a variation of PAS, quartz enhanced photoacoustic spectroscopy (QEPAS), by use of a quartz tuning fork (QTF) instead of a traditional microphone, is a booming technique for trace gas detection that has been widely used for environmental monitoring, industrial process control analysis, combustion processes, and detection of toxic and flammable gases, as well as explosives [5]. The sharply high value of the quartz tuning fork (QTF) not only facilitates the accumulation of the acoustic energy generated from the relaxation transition of gas molecules, but also makes the QEPAS based spectrophone immune to environmental noise.

Acoustic microresonators (AmRs) were usually used in QEPAS spectrophone to enhance the acoustic wave oscillation, induced by the modulated beam in the absorbing gas, by virtue of the coupling effects between the QTF and the AmRs [6–8]. Two sophisticated QEPAS spectrophones with AmRs assembled in “on-beam” and “off-beam” configurations have been developed to improve the performance of bare-QTF based QEPAS sensors [9, 10]. The spectrophone assembled in the “on-beam” configuration [9], with two AmRs positioned closely on each side of the QTF, offers a signal-to-noise ratio (SNR) enhancement factor of ~30. The spectrophone assembled in the “off-beam” configuration [10], having a single AmR with a small slit made in the middle placed alongside the QTF, can simplify optical alignment and be applied to excitation sources with a low spatial radiation quality. Recently, some novel QEPAS spectrophones were also reported. Double acoustic microresonator quartz-enhanced photoacoustic spectroscopy which employed the spectrophone that consisted of a QTF and two sets of the “on-beam” AmRs was developed for optical signal addition and multigas rapid spectral measurement with a response time of 5 ms [1]. Multi-quartz enhanced photoacoustic spectroscopy (M-QEPAS) uses a pair of QTFs with similar resonance frequencies connected in parallel, instead of a single QTF in the traditional QEPAS spectrophone, to enhance the signal amplitude through coupling effect between the two QTFs [11]. M-QEPAS realized a 1.7 times signal enhancement for the water vapor detection in the air, compared to the QEPAS sensor with a single bare QTF. But there were no AmRs configured in the M-QEPAS spectrophone.

In this paper, AmRs were added to the M-QEPAS spectrophone to further enhance the signal amplitude of the sensor. Two kinds of multi-QTF based “on-beam” QEPAS spectrophone were proposed. The resonance curves of the proposed QEPAS spectrophones were measured to determine their resonance frequencies and values. For its practical implementation, water vapor in the laboratory air was selected as the target analyte to evaluate the sensor performance in detail. The distance between the AmR and the QTF in the multi-QTF based “on-beam” QEPAS spectrophone was optimized to obtain the maximum signal amplitude.

2. Experimental Setup

The schematic diagram of the experimental setup was depicted in Figure 1. A near-infrared fiber-coupled distributed-feedback (DFB) diode laser was employed as excitation source to generate photoacoustic signals. The output wavelength of the DFB laser was 1368.69 nm, with the temperature and the current of the DFB laser set to 27°C and 80 mA. The laser wavelength can be coarsely and finely tuned by scanning the temperature and the current, respectively. A commercial ~32 kHz quartz tuning fork was used as an acoustic transducer. The laser current was modulated at ~16 kHz, corresponding to a half of the QTF resonance frequency. The output beam from the DFB laser was focused to pass through the gap between the QTF prongs by means of a fiber coupled focuser. The acoustic wave induced by the modulated laser beam effectively pushed the prongs of the QTF to vibrate. The electrical signals generated by piezoelectric effect of the QTF were processed by a transimpedance preamplifier and then were fed to a lock-in amplifier, demodulating the signal at mode and retrieving the gas concentrations.

Figure 1: Schematic of the experimental setup.

The output power and wavelength of the DFB laser as a function of current were plotted in Figure 2. The current of the DFB laser was scanned from 15 mA to 125 mA at a constant temperature of 23.95°C, corresponding to a wavelength range from 7305.8 cm⁻¹ to 7309.9 cm⁻¹. Two H₂O absorption lines, located at 7306.75 cm⁻¹ and 7308.82 cm⁻¹, were covered within the scanning range. According to the HITRAN database, the two H₂O absorption lines have the line intensities of 1.8 × 10⁻²⁰ cm/mol and 6.9 × 10⁻²² cm/mol, respectively, as shown in Figure 3(a). The relevant signal, obtained from the QEPAS sensor by use of the spectrophone based on a bare QTF, was shown in Figure 3(b). A lower detection limit can be achieved by selecting a stronger target line, but to avoid the overload of the lock-in amplifier, the weaker line at 7308.82 cm⁻¹ was selected as the target line in this experiment.

Figure 2: Output power and wavelength of the laser as a function of current.

(a)

(b)

Figure 3: (a) Locations and intensities of H₂O absorption lines from the HITRAN database; (b) signal obtained from the QEPAS sensor by use of a single bare QTF based spectrophone; SD: standard deviation.

Figure 4 shows four different QEPAS spectrophones: (a) single bare QTF based spectrophone, (b) traditional single QTF based “on-beam” spectrophone, and (c), (d) multi-QTF based “on-beam” spectrophones. In Figure 4(c), two QTFs were placed in a line with a gap of 20 μm, and two AmRs were positioned closely on the one side of each QTFs with the same gap of 20 μm. The distance from the top of the QTF prongs to the center of the AmRs was 0.7 mm. In Figure 4(d), an additional QTF was added to a traditional single QTF based “on-beam” spectrophone. The distance from the top of the QTF prongs to the center of the AmRs and the gaps between the QTF #3 and the AmRs were the same as in Figure 4(c). This configuration is equivalent to two traditional half “on-beam” spectrophones connected in series [12]. The geometric parameters of all the AmRs used in Figures 4(b)–4(d) are the same as in [13].

(a)

(b)

(c)

(d)

Figure 4: (a) Single bare QTF based spectrophone, (b) single QTF based “on-beam” spectrophone, and (c), (d) multi-QTF based “on-beam” spectrophones. The geometric parameters of all the AmRs used in Figure 4 are 4.4 mm in length and 0.6 mm in inner diameters, respectively.

3. Results and Discussion

A function generator was used to generate sinusoidal waves to excite the QTF, and the output signals of the QTF at different excitation frequencies were recorded as the resonance curves. The resonance frequency and value of the QTF can be obtained from Lorentz fitting of the square of the resonance curve [14]. The value is defined as , where represents the full width at half maximum (FWHM) of the resonance curve. The resonance curve of the single bare QTF based spectrophone (Figure 4(a)) and the traditional single QTF based “on-beam” spectrophone (Figure 4(b)) were shown in Figure 5. The frequency of the sinusoidal wave from the function generator was scanned from 32720 Hz to 32780 Hz with peak to peak amplitude of 317 mV. A standard QTF has the resonance frequency of 32768 Hz and value of 80,000–100,000 in a sealed vacuum metallic package. The frequency and the value decreased to 32748.8 Hz and 8396 in the air, after removal of the metallic housing. With the traditional single QTF based “on-beam” QEPAS spectrophone, the factor further decreased to 3193, due to the strong coupling effect between the QTF and AmRs. The lower value means more acoustic energy exchange and storage between the QTF and the AmRs.

Figure 5: Resonance curves of a single bare QTF based spectrophone and a traditional single QTF based “on-beam” spectrophone measured at atmospheric pressure in the air.

The performance of the multi-QTF based “on-beam” spectrophone shown in Figure 4(c) was first evaluated. The resonance curves of both QTFs were measured independently, and the corresponding parameters were listed in Table 1. QTFs #1 and #2 showed the approximate frequency. As a result, only one peak value on the response curve was observed, after connecting the electrodes of the two QTFs in parallel. The value of 5660 and 2923 for each QTF indicated that both the QTFs were coupled with the AmRs independently. Due to the strong coupling effect between the multi-QTF and the AmRs, the multi-QTF based “on-beam” spectrophone, shown in Figure 4(c), exhibited a value of 6918. Figure 6 shows the resonance curves obtained for QTF #1, QTF #2, and multi-QTF using the configuration of Figure 4(c), indicating that when two QTFs were connected in parallel and strongly coupled with the AmRs, -factor of multi-QTFs can be higher than each of the two QTFs.

Table 1: Parameters of multi-QTF based “on-beam” spectrophone (Figure 4(c)).

QTF #1
QTF #2
Multi-QTF

Resonance frequency (Hz)
32747.29
32744.15
32746.93

value
5660
2923
6918

Figure 6: Resonance curves obtained for QTF #1, QTF #2, and Multi-QTF using the configuration of Figure 4(c).

The modulation depth of the laser was optimized with the bare QTF based spectrophone. The laboratory air containing 1.26% H₂O was selected as the target analyte. The signal amplitudes and spectral profiles of the QEPAS signal as a function of laser modulation depth were plotted in Figures 7(a) and 7(b). As shown in Figures 7(a) and 7(b), with the modulation depth increasing from 5 to 20 mA, both the amplitude and spectra width of the QEPAS signal increased monotonously. However, with the modulation depth increasing from 13 to 20 mA, the signal amplitude increased only 9.4% (from 1.71 mV to 1.96 mV), shown in inset (j), but the spectra width increased 43.6% (from 0.44 cm⁻¹ to 0.63 cm⁻¹), shown in inset (i). Therefore, an optimum modulation depth of 13 mA was selected, considering the spectral broadening.

(a)

(b)

Figure 7: (a) QEPAS signal amplitudes as a function of laser modulation depth; (b) spectral broadening widths of QEPAS signal as a function of laser modulation depth.

QTFs #1 and #2 were first evaluated independently. The obtained signals were demonstrated in Figure 8(a). QTFs #1 and #2 showed the signal amplitudes of 41.5 mV and 37.5 mV which are 23.3 times and 21 times higher than that of the single bare QTF based spectrophone. This indicates that both QTFs #1 and #2 were strongly coupled with the AmRs assembled in the “on-beam” configuration. The QEPAS signal, obtained with the two QTFs’ electrodes connected in parallel, was also plotted in Figure 8(a). As a result, the multi-QTF based “on-beam” spectrophone showed the signal amplitude of 58.8 mV, yielding a 1.4 times enhancement compared to the traditional single QTF based “on-beam” spectrophone and a 33 times enhancement compared to the single bare QTF based spectrophone. The asymmetry of the signal was due to the residual amplitude modulation of the laser [15].

(a)

(b)

Figure 8: (a) Performance of multi-QTF based “on-beam” spectrophone shown in Figure 4(c); (b) performance of multi-QTF based “on-beam” spectrophone shown in Figure 4(d).

The performance of the multi-QTF based “on-beam” spectrophone in Figure 4(d) was evaluated in the same way. The comparisons in the resonance curves and the signal amplitudes were shown in Table 2 and Figure 8(b), respectively. In contrast with the spectrophone in Figure 4(c), the multi-QTF based “on-beam” spectrophone in Figure 4(d) generated a signal amplitude of 65.1 mV which is 1.6 times higher than that of the traditional single QTF based “on-beam” spectrophone and 36 times higher than that of the single bare QTF based spectrophone. Considering the higher signal gain, the multi-QTF based “on-beam” spectrophone in Figure 4(d) is preferred.

Table 2: Parameters of multi-QTF based “on-beam” spectrophone (Figure 4(d)).

QTF #3
QTF #4
Multi-QTF

Resonance frequency (Hz)
32744.93
32746.96
32745.68

value
5384
5540
5714

The QEPAS signal amplitude of the multi-QTF based “on-beam” spectrophone (Figure 4(d)) as a function of distance between QTF #4 and AmR #4 was optimized and shown in Figure 9. With the distance increasing from 10 to 50 μm, the signal amplitudes achieve the maximum value of 65.1 mV at the distance of 40 μm, as shown in the inset of Figure 9. This observed behavior is due to the coupling effect of the acoustic wave fields between QTF #4 and the AmRs. The signal-to-noise ratio (SNR) of the sensor can be calculated from the signal maximum value and the noise background level obtained by tuning the laser wavelength far away from the H₂O absorption lines. With the noise of 4.6 × 10⁻⁵ V, the SNR of the multi-QTF based “on-beam” spectrophone (Figure 4(d)) is 1410, corresponding to a detection limit of 9.96 ppm. Normalized to the excitation power of 5.4 mW and the detection bandwidth of 0.125 Hz, the obtained normalized noise equivalent absorption (NNEA) coefficients were 1.24 × 10⁻⁹ W·cm⁻¹·Hz−1/2.

Figure 9: Signal amplitudes of the multi-QTF based “on-beam” spectrophone (Figure 4(d)) as a function of distance between QTF #4 and AmR #4.

4. Conclusions

Acoustic microresonators are added to the most recently developed multi-QTF based QEPAS sensor to further enhance the signal amplitude. Two kinds of multi-QTF based spectrophones with “on-beam” AmR configurations were experimentally investigated and discussed. Compared with the traditional single QTF based “on-beam” spectrophone, the developed multi-QTF based “on-beam” spectrophone had a signal enhancement of 1.6 times at the same operating conditions, with the approximate noise level. A normalized equivalent absorption coefficient () of 1.24 × 10⁻⁹ W·cm⁻¹·Hz−1/2 was obtained for water vapor detection at normal atmospheric pressure. The signal enhancement can be further improved by using a phase shifter to adjust the possible phase difference between the multi-QTFs.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

The work was supported by the 973 program (Grant no. 2012CB921603), the National Natural Science Foundation of China (Grant nos. 61575113, 61275213, 61108030, 61475093, 61127017, 61178009, 61378047, and 61205216), the National Key Technology R&D Program (2013BAC14B01), the Shanxi Natural Science Foundation (2013021004-1), and the Shanxi Scholarship Council of China (2013-011, 2013-01).

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