Quantitative determination of multiple transient species is critical in investigating reaction mechanisms and kinetics under various conditions. Dual-comb spectroscopy, a comb-laser-based multi-heterodyne interferometric technique that enables simultaneous achievement of broadband, high-resolution, and rapid spectral acquisition, opens a new era of time-resolved spectroscopic measurements. Employing an electro-optic dual-comb spectrometer with central wavelength near 3 µm coupled with a Herriott multipass absorption cell, here we demonstrate simultaneous determination of multiple species, including methanol, formaldehyde, HO2 and OH radicals, and investigate the reaction kinetics. In addition to quantitative spectral analyses of high-resolution and tens of microsecond time-resolved spectra recorded upon flash photolysis of precursor mixtures, we determine a rate coefficient of the HO2 + NO reaction by directly detecting both HO2 and OH radicals. Our approach exhibits potential in discovering reactive intermediates and exploring complex reaction mechanisms, especially those of radical-radical reactions.
Time-resolved infrared spectroscopy plays an essential role in atmospheric, biological, and combustion chemistry studies, providing both temporal and spectral resolution for the identification of unstable molecules with unique vibrational spectral features and the observation of time-dependent spectral variations of multispecies reaction processes. In the molecular fingerprint region, the step-scan Fourier transform infrared (ss-FTIR) spectrometer1 has been recognized as a powerful tool with broadband spectral measurement capability, which allows it to record several vibrational bands simultaneously and thus provide decisive information for molecular identification2,3. However, the conventional ss-FTIR spectrometer requires extremely long measurement times for acquiring a time-resolved spectrum with adequate spectral resolution and sensitivity, making it difficult to use for kinetic studies. By contrast, sensitive detection of transient species can be achieved by using infrared continuous wave (cw) lasers coupled with the multipass absorption cell or wavelength modulation technique4,5. Although multispecies monitoring may be implemented by coupling several cw lasers into a system, each probe only provides the time-dependent absorption signals at a single wavelength. Hence, it is still challenging to study complex reaction system and ensure probing the targeted absorption lines without any interference from other species under various conditions.
In recent years, direct frequency comb spectroscopy (DFCS) techniques6,7,8,9,10,11, which enable high resolution, rapid, and broadband measurements, have been developed for different spectral regions and used in various applications. Time-resolved spectroscopy based on DFCS methods has been used for monitoring spectral variations under flash photolysis12, electric discharge13, laser-induced plasma14,15, and combustion conditions16 as well as for studying gas-phase reaction kinetics17,18,19, protein dynamics20, and population relaxation processes21. In particular, time-resolved DFCS methods can be demonstrated in the mid-infrared (MIR) region to achieve sensitive molecular identification and quantitation12,13,17,18,19,20. For instance, a MIR virtually imaged phased array (VIPA) spectrometer with a spectral coverage of 65 cm−1 and an optical resolution of 1 GHz (approximately 0.033 cm−1) has been employed for studying the OD + CO reaction and recording the vibrational spectra of DOCO radicals12,17,18. In that scheme, the temporal resolution can be set down to tens of microseconds; however, it may be limited by the camera integration time. In addition, the spectral resolution of approximately 0.03 cm−1 is restricted by the properties of elements, including the VIPA etalon, grating and camera, inside the spectrometer. Two identical femtosecond optical parametric oscillator combs with a spectral region of 3.15−3.45 μm has been used to observe the time-dependent phenomena of a CH4/He gas mixture under discharge13. A spectral resolution of 6 GHz (0.2 cm−1) and a temporal resolution of 20 μs can be achieved through the conventional Fourier transformation. However, the mode-locked-laser-based MIR dual-comb spectrometer is relatively complex and difficult to operate. A quantum cascade laser (QCL) based dual-comb spectrometer (QCL-DCS) with a spectral coverage of 55 cm−1 around 8.2 μm has been used for studying the single-shot spectra and kinetics of protein reactions20. The dual-comb spectra were recorded with a spectral resolution of a few wavenumbers at sub-microsecond time resolution and compared with the ss-FTIR spectra. The QCL-DCS has been presented with a compact system;19,20 nevertheless, it may be more suitable for time-resolved measurements at relatively low spectral resolution due to the large comb mode spacing (approximately 0.3 cm−1) of QCLs.
To investigate rotationally resolved spectra and study gas-phase reaction kinetics with distinguishing probes of multiple species, the spectral resolution of the time-resolved spectrometer must be higher than the observed absorption line width. In the 3-μm spectral region, the absorption line width of most molecules is typically a few hundred MHz at low pressure (<100 Torr) and room temperature, and the absorption line width depends on the effects of Doppler and pressure broadenings. In time-resolved dual-comb spectroscopy, a trade-off exists among the spectral resolution, temporal resolution, and spectral coverage of the frequency combs. Although dual-comb system with mode-locked or quantum cascade lasers can offer a wide measurement range without wavelength sweep, the system is unable to achieve high spectral resolution (<0.01 cm−1) at adequate temporal resolution (tens of microseconds) for simultaneously distinguishing multiple reaction intermediates.
In this article, we report high-resolution time-resolved dual-comb spectroscopy for simultaneous determination of multiple reaction species and kinetic studies of the HO2 + NO reaction, which is one of the most important reactions in atmospheric chemistry22,23. The reaction of HO2 radicals with NO, leading to the formation of OH radicals and NO2, plays a critical role in the O3 formation cycle24,25. To investigate the HO2 + NO reaction, we first record the time-resolved spectra of the HO2 radicals near 3 μm by employing an electro-optic dual-comb spectrometer coupled with a Herriott reaction cell upon ultraviolet photolysis of the precursor mixtures. Multiple reaction species, including the precursor (methanol, CH3OH), the stable product (formaldehyde, H2CO), and HO2 radicals, are observed and distinguished based on rotationally resolved spectra and distinct temporal profiles. Moreover, simultaneous measurements of CH3OH, HO2, H2CO, and OH signals are achieved by recording the time-resolved spectra at around 3422 cm−1. Hence, the kinetics of the HO2 + NO reaction can be studied through the direct detection of both HO2 and OH radicals and the rate coefficient of the HO2 + NO reaction can be derived by model fitting of the temporal absorbance profiles of HO2 and OH radicals under different experimental conditions.
High-resolution time-resolved dual-comb spectroscopy
The high-resolution time-resolved absorption spectroscopy was performed by means of an electro-optic dual-comb system coupled with a Herriott flow cell, as illustrated in Fig. 1. Our MIR dual-comb system was constructed using a pair of electro-optic combs at 1050 nm and a tunable cw laser (765−800 nm) with difference frequency generation (DFG)26. An excimer laser operating at 1 Hz was used for the flash photolysis of the precursor mixtures to generate free radicals. The MIR dual-comb laser beam was passed through the Herriott multipass flow reactor and then detected by a photovoltaic HgCdTe (MCT) detector. Afterwards, dual-comb interferograms were recorded and digitized with a 12-bit data-acquisition (DAQ) board at a sampling rate of 500 MS s−1. To monitor the time-dependent spectral evolution upon the irradiation of the flowing mixtures, both excimer laser and DAQ board were synchronized with the dual-comb interference signal. In addition, the external trigger of the excimer laser was set to have a time delay by using a pulse delay generator. Additional details of the experimental setup are shown in Methods.
To perform high-resolution time-resolved spectroscopy based on comb-mode-resolved dual-comb technique, we first continuously recorded dual-comb interference signal over tens of milliseconds. The time-domain dual-comb signal was cut every few interferograms and separately Fourier-transformed to generate time-dependent comb-mode-resolved spectra. In the comb-mode-resolved dual-comb technique, each comb line provides one spectral sampling point. The detailed descriptions are provided in Supplementary Note 1 and Supplementary Fig. 1. After Fourier transformation of the time-dependent dual-comb interferograms and data processing with programs, a precursor transmission spectrum before photolysis and time-resolved signal transmission spectra after photolysis can be obtained. Typically, the sample point spacing corresponds to the comb mode spacing, and can be decreased by interleaving. The temporal resolution can be adjusted according to the number of interferograms used to generate each signal spectrum.
Simultaneous determination of multiple reaction species near 3 μm
To demonstrate high-resolution time-resolved dual-comb spectroscopy, we measured the time-dependent difference absorbance spectra upon the flash photolysis of a flowing mixture of (COCl)2/CH3OH/O2 (1/1.5/20.6) at 4.53 Torr and 296 K, as shown in Fig. 2. The dual-comb spectrometer was set with a comb mode spacing (frep) of 146 MHz (~4.87 × 10−3 cm−1) and a different repetition frequency (δf) of 0.05 MHz. The time-dependent difference absorbance spectra were derived using the following equation: −ln[Tn(ν) / T0(ν)], where Tn(ν) represents the signal transmission spectra taken after photolysis and T0(ν) represents the precursor transmission spectrum taken before photolysis. Each time-dependent spectrum was obtained through the Fourier transformation of 20 interferograms and averaged over 1000 excimer laser shots. The temporal resolution of the time-resolved spectra was estimated to be 400 μs. To perform transient absorption measurements for the HO2 radicals, oxalyl chloride (COCl)2 was used as the precursor to efficiently generate Cl atoms upon irradiation with the excimer laser at 248 nm. The Cl atoms reacted with methanol (CH3OH) through hydrogen atom abstraction to form HCl and CH2OH radicals. Subsequently, CH2OH mainly reacted with excessive O2 in the system to produce formaldehyde (H2CO) and hydroperoxyl radical (HO2). The difference absorbance signals from CH3OH, H2CO, and HO2 radicals were simultaneously obtained and distinguished by their distinct temporal profiles (Supplementary Fig. 2).
Figure 3 shows a comparison of the measured spectra and predicted transition lines of HO2 and H2CO in the region 3413.5−3417.5 cm−1. Figure 3a depicts the absorbance spectrum of the precursor obtained before flash photolysis. At an early period after flash photolysis of the flowing mixture, several absorption lines from the stable product (H2CO) and transient HO2 radicals were observed, as illustrated in Fig. 3b. Most of the absorption lines in Fig. 3b can be assigned to the transitions of the ν1 band of HO227 and the 2ν2 band of H2CO28. A simulated spectrum of HO2 taken from the HITRAN database29 is depicted in Fig. 3d, and a spectrum of H2CO generated by the PGOPHER program30 with the vibrational-rotational parameters of the 2ν2 band of H2CO28 is presented in Fig. 3e. The absorbance intensities of the HO2 radicals reduced mainly due to the self-reaction of HO2 radicals with a rate coefficient of 1.7 × 10‒12 cm3 molecule‒1 s‒1 at 296 K31. These HO2 lines exhibited considerably weak absorption signals after tens of milliseconds, as displayed in Fig. 3c. In addition, several additional absorption lines (indicated with a black asterisk in Fig. 3b) were found with the similar temporal profiles as that of the HO2 ν1 transitions, as shown in Supplementary Fig. 3. Although these additional lines have never been observed under a discharge system in previous studies, we tentatively assigned them to the hot band transitions of HO2 according to anharmonic frequency calculations (B3LYP/aug-cc-pVTZ). The calculated center frequencies of the HO2 vibrational bands are listed in Supplementary Table 1. The center frequencies of the (110)-(010) and (101)-(001) hot bands of HO2 were calculated with red shifts of 16.7 and 3.8 cm−1, respectively, from the ν1 fundamental band. Each vibrational band may include hundreds of ro-vibrational transitions. To fully assign these additional absorption lines and obtain the ro-vibrational parameters of each band, spectral acquisition would be conducted over the spectral range from 3350 to 3500 cm−1 in future work.
To perform quantitative spectral analysis and estimate the concentration of HO2 radicals, we selected Cl2 as the precursor to produce Cl atoms upon 351-nm photolysis and studied the time-resolved spectra of the HO2 radicals with well-known reaction mechanisms. Figure 4 illustrates the difference absorbance spectra of the HO2 radicals obtained at 0–0.1 ms after the laser photolysis of a flowing mixture of Cl2/CH3OH/O2 (1/0.9/58, 5.94 Torr, 296 K). To increase the spectral sampling points, we recorded the time-resolved dual-comb spectra by using different comb mode spacings. The interleaved spectrum of the HO2 radicals was curve-fitted using a multi-peak Voigt function with a fixed Gaussian width (full width at half maximum [FWHM]) of 220 MHz (which corresponded to Doppler width at 296 K). The Lorentzian width (FWHM) was obtained to be 51 ± 2 MHz, which is comparable to the value of 50 MHz estimated using a broadening coefficient γair (half width at half maximum [HWHM]) of 0.107 cm−1 atm−1 29. The line strengths of the HO2 transitions were estimated and compared with the values tabulated in the HITRAN database, as listed in Supplementary Table 2. The obtained line strengths were three times higher than those from the HITRAN database29,32. In addition, in a recent experiment for line strength measurements of the HO2 ν3 band under a flash photolysis system, the obtained line strengths were reported to be approximately three times higher than those from previous studies33.
Kinetic studies of the HO2+NO reaction
To investigate the kinetics of the HO2 + NO reaction, we first recorded the time-resolved dual-comb spectra upon irradiation of a flowing mixture of Cl2/CH3OH/O2/NO (1/0.14/10.02/0.017, 6.02 Torr, 296 K) at 351 nm, as shown in Fig. 5. The dual-comb spectrometer was set with a comb mode spacing of 181 MHz (~6.03 × 10−3 cm−1) and a different repetition frequency of 0.08 MHz. Each time-dependent spectrum was generated by Fourier transformation of 10 dual-comb interferograms and averaged over 1600 excimer laser shots. By recording time-resolved spectra at around 3422 cm−1, both HO2 and OH radicals were simultaneously detected, which is useful for kinetic studies under various experimental conditions.
A comparison of the observed spectra and predicted transition lines of HO2, H2CO, and OH in the region 3421.75−3422.45 cm−1 is displayed Fig. 6. An absorbance spectrum recorded before photolysis of a flowing mixture of Cl2/CH3OH/O2 (1/0.36/24.5, 8.24 Torr, 296 K) and a difference absorbance spectrum recorded at 0–0.1 ms after photolysis are depicted in Fig. 6a, b, respectively. In this spectral region, several additional lines indicated with a black asterisk in Fig. 6b were observed and tentatively assigned to be HO2 hot band lines according to comparison of the temporal profiles (Supplementary Fig. 4). With the addition of NO in the flow cell, two lines belonging to the absorption of OH radicals were clearly observed without interference with other reaction products, as shown in Fig. 6c. For the kinetic studies, to avoid possible interferences with the H2CO and HO2 hot band absorption lines, a HO2 line at 3422.102 cm‒1 and two OH lines at 3421.932 and 3422.014 cm‒1 were selected for the analysis of temporal absorbance profiles at different experimental conditions.
In kinetic measurements, we first analyzed the time-resolved dual-comb spectrum without the addition of NO to the reaction system and determined the initial concentration of Cl atoms through the model-fitting of the absorbance time trace of HO2 lines. With the addition of NO in reaction system, the rate coefficients of the HO2 + NO reaction were obtained by analyzing the temporal absorbance profiles of HO2 and OH radicals with the kinetic model (Supplementary Table 3). Figure 7a shows a representative time trace of the HO2 line at 3422.102 cm‒1 taken from the time-resolved spectra, which were measured upon photolysis of a flowing mixture of Cl2/CH3OH/O2/N2 (1/0.45/25.7/7.18, 8.33 Torr, 296 K) and obtained with a sample point spacing of 203 MHz (~6.77 × 10−3 cm−1) and a temporal resolution of 50 μs. The signal to noise ratio (SNR) of this time trace was estimated to be approximately 50 over 1600 photolysis laser shots. The yellow solid line represents the curve that was fitted using the kinetic model. The initial concentration of Cl atoms was determined to be 2.81 × 1013 molecules cm−3. When [NO]0 = 3.06 × 1014 molecules cm−3 in the reaction system, the temporal absorbance profiles of the HO2 and OH lines (indicated with blue and red lines, respectively, in Fig. 7b) were recorded simultaneously and analyzed for determining the first-order rate coefficients for the reaction of HO2 with NO. Furthermore, the line strengths of the OH transitions were estimated by analyzing the spectral profiles (Supplementary Fig. 6). The obtained line strength of the OH transitions (S = (1.9 ± 0.6) × 10‒20 cm molecule‒1) is comparable to the value tabulated in the HITRAN database (S = (2.6 ± 0.5) × 10‒20 cm molecule‒1)29,34.
We conducted 17 measurements under total pressures of approximately 8.5 and 17 Torr with [Cl2] = (1.7 − 10.4) × 1015 molecules cm−3, [CH3OH] = (2.9 − 3.8) × 1015 molecules cm−3, [O2] = (1.7 − 2.5) × 1017 molecules cm−3, [Cl]0 = (1.1 − 4.3) × 1013 molecules cm−3, and [NO]0 = (1.3 − 4.5) × 1014 molecules cm−3 at 296 K. Several lines of HO2 and OH radicals in the measured time-resolved spectra were selected and analyzed through kinetic model fitting. The bimolecular rate constant of the HO2 + NO reaction was derived from the fitted slope of the dependence of the first-order rate coefficient (kI) on [NO]0, as shown in Fig. 8. The details of each experimental condition and the fitted kI values are listed in Supplementary Table 4. Considering the slope fitting error (3.4 %) and some errors in the measurements of the flow rates (3 %), temperature (1 %), and pressure (1 %), we estimated the overall standard error to be ~5%. Therefore, the rate coefficient for HO2 + NO was determined to be (8.7 ± 0.4) × 10‒12 cm3 molecule‒1 s‒1. This result is in agreement with those of other experimental reports25,35,36, thus, the adopted method using time-resolved dual-comb spectroscopy is feasible for kinetic studies.
We simultaneously demonstrated multispecies determination under gas-phase chemical reaction systems and studied the kinetics of the HO2 + NO reaction by employing time-resolved dual-comb spectroscopy near 3 μm. Quantitative spectral and temporal analyses of the recorded time-resolved dual-comb spectra were performed. The advantage of utilizing the adopted approach for kinetic studies is that we can first record time-dependent dual-comb interferograms and then analyze the Fourier-transformed spectra with different temporal resolutions. A comparison of the temporal profiles of a HO2 line at 3415.663 cm−1 with temporal resolutions of 25 and 400 μs is displayed in Supplementary Fig. 7a. The SNRs of the time traces with temporal resolutions of 25 and 400 μs were estimated to be 240 and 929, respectively, over 4000 excimer laser shots. Supplementary Fig. 7b shows an evolution of the SNR of the temporal profiles with a temporal resolution of 25 μs as a function of the average number of spectra. The detection limit for the HO2 absorption line at 3415.663 cm−1 was estimated to be 2.5 × 1011 molecules cm−3 (with a temporal resolution of 25 μs and average of 4000 shots). Although the sensitivity of current system for HO2 detection is lower than that attained in experiments using cavity ring-down spectroscopy in the near infrared region37,38, the sensitivity of the adopted method can be improved by coupling the dual-comb laser with a cavity-enhanced reaction cell.
By employing the dual-comb spectrometer in the spectral region of the fundamental OH stretch, we simultaneously determined HO2 and OH radicals as well as CH3OH molecules. Thus, our adopted method may be suitable for studying the reaction between hydroxyl and methylperoxy radicals39,40,41 and directly obtaining the yield of methanol from the OH + CH3O2 reaction. For a rough estimation, both methanol and OH radicals may be detected with a detection limit of approximately 1 × 1011 molecules cm−3 by recording time-resolved spectra at around 3650 cm−1.
Moreover, our electro-optic dual-comb spectrometer can be designed with an all-fiber compact system without any complicated phase-lock electronics. Thus, the proposed method is promising for in situ time-resolved measurements and remote sensing to explore the issues in atmospheric chemistry and other applied sciences. Future studies can perform quantitative spectral analysis with rotationally resolved spectra of key radicals, such as organic peroxy radicals (RO2) with torsion-CH stretch coupled infrared spectral features42. Unstable molecules, such as the simplest Criegee intermediate2, which has relatively weak C-H vibrational bands, can also be observed with our time-resolved dual-comb spectrometer coupled with a cavity-enhanced cell.
MIR time-resolved dual-comb spectroscopy
Our MIR electro-optic dual-comb spectrometer is setup using difference frequency generation between a 30 ps electro-optic dual-comb laser at 1050 nm and a widely tunable cw laser in the region 765 − 800 nm26. The spectral tunable range of the MIR dual-comb laser is from 2976 to 3548 cm−1, and the spectral tunable range can be extended by simply changing the cw lasers. The MIR dual-comb source has a spectral span of 1.8 cm−1 and an average power of up to a few mW. The sample point spacing can be adjusted by changing the comb mode spacing, which can be simply tuned from 80 MHz to 4 GHz by adjusting the frequency of the signal generators. All of signal generators and the DAQ board are referenced to a GPS disciplined rubidium clock.
To perform time-resolved dual-comb spectroscopy, the photolysis laser and the DAQ board are synchronized with a multi-channel pulse delay generator, which is triggered by the obtained dual-comb multi-heterodyne signals. Time-domain dual-comb interferograms can thus be continuously recorded before and after excimer laser irradiation. The total acquisition time is 64 ms at a sampling rate of 500 MS s−1. The temporal resolution of the adopted method is adjustable and depends on the interferogram length used to generate each signal spectrum. The minimum acquisition time for the generation of a comb-mode-resolved spectrum is the inverse of the different repetition frequency (δf) in the dual-comb system. Therefore, the dual-comb spectrometer can be used to study fast reactions or detect intermediates with a temporal resolution of <1 μs and a sample point spacing >0.008 cm−1 26. In the experiments, each time-dependent spectrum is obtained through Fourier transformation of at least five interferograms. The detailed description of data processing is presented in Supplementary Note 1. For absolute frequency calibration, the time-resolved spectra of the reaction cell and the dual-comb spectra of a N2O reference cell are simultaneously measured. The wavenumbers of the recorded dual-comb spectra are calibrated based on the simulated spectra of N2O molecules obtained from the HITRAN database29. Thus, the accuracy of absolute frequency measurements is expected to be <30 MHz (0.001 cm−1). More precise calibration can be achieved by measuring frequencies of the cw lasers with a metrology comb system10.
Herriott multipass reaction cell
The Herriott cell consists of a pair of 2-inch concave mirrors with a 25-mm-diameter center hole and 4.75-mm-diameter off-axis hole in each mirror for passage of the ultraviolet (UV) photolysis beam and MIR dual-comb beam, respectively. The MIR dual-comb beam is coupled into the cell and then multi-reflected between the two mirrors separated by a distance of 655 mm. The Herriott cell is designed to allow 63 passes of the MIR beam. A total path length is determined to be (41.8 ± 0.6) m and the length of overlap between the UV and MIR beams is estimated to be (24.5 ± 5.9) m (Supplementary Note 2 and Supplementary Fig. 5). To generate HO2 radicals and study the HO2 + NO reaction, we performed flash photolysis of flowing mixtures of (COCl)2 or Cl2/CH3OH/O2/N2/NO. The flow rates of each precursor are controlled using calibrated mass flow controllers. A small stream of N2 or O2 is used to purge the Herriott mirrors. The total flow rates are typically >1300 standard cm3 min−1 at low total pressure (< 10 Torr). The partial pressures of each precursor in the Herriot cell are calculated according to the ratios of the flow rates and the total pressure.
The data supporting the findings of this study are available within the article and its Supplementary Information and from the corresponding author upon reasonable request.
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This project is supported by Ministry of Science and Technology, Taiwan (grant no. 108-2112-M-001-001-MY3 and grant no.108-2639-M-009 -001 -ASP) and Academia Sinica.
The authors declare no competing interests.
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Luo, PL., Horng, EC. Simultaneous determination of transient free radicals and reaction kinetics by high-resolution time-resolved dual-comb spectroscopy. Commun Chem 3, 95 (2020). https://doi.org/10.1038/s42004-020-00353-6