Pin-yi WANG, Fu WAN, Jian-xin WANG, et al. Trace gas detection using cavity-enhanced Raman spectroscopy with injection locking[J]. Optics and precision engineering, 2018, 26(8): 1917-1924.
DOI:
Pin-yi WANG, Fu WAN, Jian-xin WANG, et al. Trace gas detection using cavity-enhanced Raman spectroscopy with injection locking[J]. Optics and precision engineering, 2018, 26(8): 1917-1924. DOI: 10.3788/OPE.20182608.1917.
Trace gas detection using cavity-enhanced Raman spectroscopy with injection locking
In order to improve the Raman scattering intensity of a trace gas
a cavity-enhanced Raman spectroscopy (CERS) technique with injection locking was introduced. A diode laser input (638 nm
15 mW) was coupled into a V-shaped enhanced cavity composed of three highly reflective mirrors. Using the injection locking technique
an intracavity laser beam was generated and enhanced by a factor of 500 to obtain a power of 7.5 W. The Raman spectra of the individual trace gases and the mixture were obtained. According to the principle of Raman spectrum peak selection and a signal-to-noise ratio greater than 3
the characteristic Raman peaks of H
2
CO
CO
2
CH
4
C
2
H
6
C
2
H
4
and C
2
H
2
are determined as 4 156
2 143
1 388
2 918
2 955
1 344
and 1 975 cm
-1
respectively
and the limits of detection are determined as 10.2
21.7
9.4
2.1
8.9
4.9
and 3.3 Pa. Trace homonuclear diatomic gases and mixed gases can thus be detected simultaneously using a single-wavelength diode laser and CERS. Therefore
CERS has the potential to become an alternative optical technology for gas detection.
关键词
Keywords
references
CAMPBELL E K, HOLZ M, MAIER J P, et al.. Gas phase absorption spectroscopy of C+60 and C+70 in a cryogenic ion trap:comparison with astronomical measurements[J]. Astrophysical Journal, 2016, 822(1):17.
MICHELUCCI U, VENTURINI F. Novel semi-parametric algorithm for interference-immune tunable absorption spectroscopy gas sensing[J]. Sensors, 2017, 17(10):2281.
WOJTAS J, GLUSZEK A, HUDZIKOWSKI A, et al.. Mid-infrared trace gas sensor technology based on intracavity quartz-enhanced photoacoustic spectroscopy[J]. Sensors, 2017, 17(3):513.
WANG Q, WANG Z, CHANG J, et al.. Fiber-ring laser-based intracavity photoacoustic spectroscopy for trace gas sensing[J]. Optics Letters, 2017, 42(11):2114.
HECOBIAN A, YALIN A P, MCHALE L E. Open-path cavity ring-down spectroscopy for trace gas measurements in ambient air[J]. Optics Express, 2016, 24(5):5523.
CALL M, SCHULZ K G, CARVALHO M C, et al.. Technical note:Coupling infrared gas analysis and cavity ring down spectroscopy for autonomous, high-temporal-resolution measurements of DIC and δ13C-DIC[J]. Biogeosciences, 2017, 14:1-17.
RAMAN C V, KRISHNAN K S. A new type of secondary radiation[J]. Nature, 1928, 121(3048):501-502.
MALARD L M, PIMENTA M A, DRESSELHAUS G, et al.. Raman spectroscopy in graphene[J]. Physics Reports, 2009, 473(5):51-87.
F. T F, KOENIG J L. Raman spectra of graphite[J]. Journal of Chemical Physics, 1970, 53(3):1126-1130.
KNIGHT D S, WHITE W B. Characterization of diamond films by Raman spectroscopy[J]. Journal of Materials Research, 1989, 4(2):385-393.
HUNGER D, STEINMETZ T, COLOMBE Y, et al.. Fiber Fabry-Perot cavity with high finesse[J]. New Journal of Physics, 2010, 12(6):065038.
LEY M, LOUDON R. Quantum theory of high-resolution length measurement with a Fabry-Perot interferometer[J]. Optica Acta International Journal of Optics, 1987, 34(2):227-255.
LANG R. Injection locking properties of a semiconductor laser[J]. IEEE J. Quantum Electron, 1982, 18(6):976-983.
KUROKAWA K. Injection locking of microwave solid-state oscillators[J]. Proc. IEEE, 1973, 61(10):1386-1410.
KIKUCHI K, OKOSHI T, TANIKOSHI S. Amplitude modulation of an injection-locked semiconductor laser for heterodyne-type optical communications[J]. Optics Letters, 1984, 9(3):99-101.