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Shen C, Wen C, Huang X, Long X. A Versatile Multiple-Pass Raman System for Industrial Trace Gas Detection. SENSORS (BASEL, SWITZERLAND) 2021; 21:7173. [PMID: 34770478 PMCID: PMC8588027 DOI: 10.3390/s21217173] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 09/28/2021] [Revised: 10/16/2021] [Accepted: 10/26/2021] [Indexed: 11/23/2022]
Abstract
The fast and in-line multigas detection is critical for a variety of industrial applications. In the present work, we demonstrate the utility of multiple-pass-enhanced Raman spectroscopy as a unique tool for sensitive industrial multigas detection. Instead of using spherical mirrors, D-shaped mirrors are chosen as cavity mirrors in our design, and 26 total passes are achieved in a simple and compact multiple-pass optical system. Due to the large number of passes achieved inside the multiple-pass cavity, experiments with ambient air show that the noise equivalent detection limit (3σ) of 7.6 Pa (N2), 8.4 Pa (O2) and 2.8 Pa (H2O), which correspond to relative abundance by volume at 1 bar total pressure of 76 ppm, 84 ppm and 28 ppm, can be achieved in one second with a 1.5 W red laser. Moreover, this multiple-pass Raman system can be easily upgraded to a multiple-channel detection system, and a two-channel detection system is demonstrated and characterized. High utilization ratio of laser energy (defined as the ratio of laser energy at sampling point to the laser output energy) is realized in this design, and high sensitivity is achieved in every sampling position. Compared with single-point sampling system, the back-to-back experiments show that LODs of 8.0 Pa, 8.9 Pa and 3.0 Pa can be achieved for N2, O2 and H2O in one second. Methods to further improve the system performance are also briefly discussed, and the analysis shows that similar or even better sensitivity can be achieved in both sampling positions for practical industrial applications.
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Affiliation(s)
| | | | | | - Xinggui Long
- Institute of Nuclear Physics and Chemistry, China Academy of Engineering Physics, Mianyang 621900, China; (C.S.); (C.W.); (X.H.)
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Niemes S, Telle HH, Bornschein B, Fasselt L, Größle R, Priester F, Schlösser M, Sturm M, Welte S, Zeller G. Accurate Reference Gas Mixtures Containing Tritiated Molecules: Their Production and Raman-Based Analysis. SENSORS 2021; 21:s21186170. [PMID: 34577377 PMCID: PMC8473055 DOI: 10.3390/s21186170] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 07/16/2021] [Revised: 09/01/2021] [Accepted: 09/10/2021] [Indexed: 11/16/2022]
Abstract
Highly accurate, quantitative analyses of mixtures of hydrogen isotopologues—both the stable species, H2, D2, and HD, and the radioactive species, T2, HT, and DT—are of great importance in fields as diverse as deuterium–tritium fusion, neutrino mass measurements using tritium β-decay, or for photonuclear experiments in which hydrogen–deuterium targets are used. In this publication we describe a production, handling, and analysis facility capable of fabricating well-defined gas samples, which may contain any of the stable and radioactive hydrogen isotopologues, with sub-percent accuracy for the relative species concentrations. The production is based on precise manometric gas mixing of H2, D2, and T2. The heteronuclear isotopologues HD, HT, and DT are generated via controlled, in-line catalytic reaction or by β-induced self-equilibration, respectively. The analysis was carried out using an in-line intensity- and wavelength-calibrated Raman spectroscopy system. This allows for continuous monitoring of the composition of the circulating gas during the self-equilibration or catalytic evolution phases. During all procedures, effects, such as exchange reactions with wall materials, were considered with care. Together with measurement statistics, these and other systematic effects were included in the determination of composition uncertainties of the generated reference gas samples. Measurement and calibration accuracy at the level of 1% was achieved.
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Affiliation(s)
- Simon Niemes
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
- Correspondence: (S.N.); (H.H.T.)
| | - Helmut H. Telle
- Departamento de Química Física Aplicada, Campus de Cantoblanco, Universidad Autónoma de Madrid, 28049 Madrid, Spain
- Correspondence: (S.N.); (H.H.T.)
| | - Beate Bornschein
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
| | - Lucian Fasselt
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
- Institut für Physik, Humboldt-Universität zu Berlin, Unter den Linden 6, 10099 Berlin, Germany
| | - Robin Größle
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
| | - Florian Priester
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
| | - Magnus Schlösser
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
| | - Michael Sturm
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
| | - Stefan Welte
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
| | - Genrich Zeller
- Tritium Laboratory Karlsruhe (TLK), Institute for Astroparticle Physics (IAP), Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76021 Karlsruhe, Germany; (B.B.); (L.F.); (R.G.); (F.P.); (M.S.); (M.S.); (S.W.); (G.Z.)
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