Identification of hydrocarbon molecules using emission spectra of femtosecond laser-induced plasma

Hydrocarbon molecular species are identified, and their concentrations are measured using femtosecond laser-induced breakdown spectroscopy (fs-LIBS). For comparison, conventional nanosecond laser-induced breakdown spectroscopy (ns-LIBS), which is sensitive only to atom compositions and not to molecular species, is conducted simultaneously. Hydrocarbon-containing gas mixtures are prepared by mixing methane (CH<sub>4</sub>), ethylene (C<sub>2</sub>H<sub>4</sub>), propane (C<sub>3</sub>H<sub>8</sub>), carbon dioxide (CO<sub>2</sub>), oxygen (O<sub>2</sub>) and nitrogen (N<sub>2</sub>). While the molecular compositions of the mixtures vary, the atomic mole fractions of carbon (C), hydrogen (H), oxygen (O), and nitrogen (N) are kept constant within each set of prepared mixtures to evaluate the molecule detection capabilities of fs- and ns-LIBS techniques. Laser pulses from a Ti:Sapphire femtosecond laser (pulse duration 35fs) and a nanosecond-pulsed Nd:YAG laser (pulse duration 9 ns) are focused on the gas mixtures to induce laser-induced plasmas (LIP). In the fs-LIP spectra, CN violet bands (B<sup>2</sup><i>Σ</i>-X<sup>2</sup><i>Σ</i>,<i>Δ</i><i>υ</i>=0,-1,+1; 370-395 nm, 350-365 nm, 410-425 nm, respectively), C<sub>2</sub> swan bands (d<sup>3</sup><i>Π</i><sub>g</sub>-a<sup>3</sup><i>Π</i><sub>u</sub>,<i>Δ</i><i>υ</i>=0,-1,+1; 500-520 nm, 450-480 nm, 540-570 nm, respectively), and a CH radical peak (A<sup>2</sup><i>Δ</i>-X<sup>2</sup>Π; 430 nm) are observed, which are sensitive to the molecular composition. Conversely, all the ns-LIP spectra, dominated by atomic emission lines, are nearly identical when the atomic fractions are fixed while varying the molecular composition. This is likely due to the ns-LIP completely dissociating the molecules in it with the inverse-Bremsstrahlung (IB) photon absorption by densely populated electrons. For reduced-order analyses of the spectra, proper orthogonal decomposition (POD) is used, while support vector regression (SVR) and support vector classification (SVC) models are employed for the calibration of the atomic concentrations and the identification of molecular species, respectively.

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Publication Details

Journal
Optics Express
Published
2025-05-23
DOI
https://doi.org/10.1364/oe.558919
Citations
1
Primary Topic
Laser-induced spectroscopy and plasma
Type
article
Field-Weighted Citation Impact
0.86

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article

Identification of hydrocarbon molecules using emission spectra of femtosecond laser-induced plasma

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1 citations
Optics Express
Laser-induced spectroscopy and plasma
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article

Identification of hydrocarbon molecules using emission spectra of femtosecond laser-induced plasma

K. Kim, Hyungrok Do, Jongwun Choi, Min‐Jung Kang, Wonjik Shin, Hyunseung Rhee
article en
1 citations

Abstract

Hydrocarbon molecular species are identified, and their concentrations are measured using femtosecond laser-induced breakdown spectroscopy (fs-LIBS). For comparison, conventional nanosecond laser-induced breakdown spectroscopy (ns-LIBS), which is sensitive only to atom compositions and not to molecular species, is conducted simultaneously. Hydrocarbon-containing gas mixtures are prepared by mixing methane (CH<sub>4</sub>), ethylene (C<sub>2</sub>H<sub>4</sub>), propane (C<sub>3</sub>H<sub>8</sub>), carbon dioxide (CO<sub>2</sub>), oxygen (O<sub>2</sub>) and nitrogen (N<sub>2</sub>). While the molecular compositions of the mixtures vary, the atomic mole fractions of carbon (C), hydrogen (H), oxygen (O), and nitrogen (N) are kept constant within each set of prepared mixtures to evaluate the molecule detection capabilities of fs- and ns-LIBS techniques. Laser pulses from a Ti:Sapphire femtosecond laser (pulse duration 35fs) and a nanosecond-pulsed Nd:YAG laser (pulse duration 9 ns) are focused on the gas mixtures to induce laser-induced plasmas (LIP). In the fs-LIP spectra, CN violet bands (B<sup>2</sup><i>Σ</i>-X<sup>2</sup><i>Σ</i>,<i>Δ</i><i>υ</i>=0,-1,+1; 370-395 nm, 350-365 nm, 410-425 nm, respectively), C<sub>2</sub> swan bands (d<sup>3</sup><i>Π</i><sub>g</sub>-a<sup>3</sup><i>Π</i><sub>u</sub>,<i>Δ</i><i>υ</i>=0,-1,+1; 500-520 nm, 450-480 nm, 540-570 nm, respectively), and a CH radical peak (A<sup>2</sup><i>Δ</i>-X<sup>2</sup>Π; 430 nm) are observed, which are sensitive to the molecular composition. Conversely, all the ns-LIP spectra, dominated by atomic emission lines, are nearly identical when the atomic fractions are fixed while varying the molecular composition. This is likely due to the ns-LIP completely dissociating the molecules in it with the inverse-Bremsstrahlung (IB) photon absorption by densely populated electrons. For reduced-order analyses of the spectra, proper orthogonal decomposition (POD) is used, while support vector regression (SVR) and support vector classification (SVC) models are employed for the calibration of the atomic concentrations and the identification of molecular species, respectively.

Optics ExpressVol. 33(12)
National Research Foundation of Korea, Korea Institute of Energy Technology Evaluation and Planning
Openalex Percentile: Top 30%
Laser-induced spectroscopy and plasma
0.86
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