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raman spectra and cross sections of ammonia chlorine hydrogen sulfide phosgene and sulfur dioxide toxic gases in the fingerprint region 400 1400 cm 1

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Raman spectra and cross sections of ammonia, chlorine, hydrogen sulfide, -1 phosgene, and sulfur dioxide toxic gases in the fingerprint region 400-1400 cm R L Aggarwal, L W Farrar, S Di Cecca, and T H Jeys Citation: AIP Advances 6, 025310 (2016); doi: 10.1063/1.4942109 View online: http://dx.doi.org/10.1063/1.4942109 View Table of Contents: http://aip.scitation.org/toc/adv/6/2 Published by the American Institute of Physics Articles you may be interested in RELATIVE RAMAN CROSS SECTION FOR N2, O2, CO, CO2, SO2, AND H2S AIP Advances 18, (2003); 10.1063/1.1653548 AIP ADVANCES 6, 025310 (2016) Raman spectra and cross sections of ammonia, chlorine, hydrogen sulfide, phosgene, and sulfur dioxide toxic gases in the fingerprint region 400-1400 cm−1 R L Aggarwal,a L W Farrar, S Di Cecca, and T H Jeys MIT Lincoln Laboratory, Lexington, MA 02420-9108, USA (Received 10 December 2015; accepted February 2016; published online 11 February 2016) Raman spectra of ammonia (NH3), chlorine (Cl2), hydrogen sulfide (H2S), phosgene (COCl2), and sulfur dioxide (SO2) toxic gases have been measured in the fingerprint region 400-1400 cm−1 A relatively compact (< 2′x2′x2′), sensitive, 532 nm 10 W CW Raman system with double-pass laser and double-sided collection was used for these measurements Two Raman modes are observed at 934 and 967 cm−1 in NH3 Three Raman modes are observed in Cl2 at 554, 547, and 539 cm−1, which are due to the 35/35 35/37, and 37/37 Cl isotopes, respectively Raman modes are observed at 870, 570, and 1151 cm−1 in H2S, COCl2, and SO2, respectively Values of 3.68 ± 0.26x10−32 cm2/sr (3.68 ± 0.26x10−36 m2/sr), 1.37 ± 0.10x10−30 cm2/sr (1.37 ± 0.10x10−34 m2/sr), 3.25 ± 0.23x10−31 cm2/sr (3.25 ± 0.23x10−35 m2/sr), 1.63 ± 0.14x10−30 cm2/sr (1.63 ± 0.14x10−34 m2/sr), and 3.08 ± 0.22x10−30 cm2/sr (and 3.08 ± 0.22x10−34 m2/sr) were determined for the differential Raman cross section of the 967 cm−1 mode of NH3, sum of the 554, 547, and 539 cm−1 modes of Cl2, 870 cm−1 mode of H2S, 570 cm−1 mode of COCl2, and 1151 cm-1 mode of SO2, respectively, using the differential Raman cross section of 3.56 ± 0.14x10−31 cm2/sr (3.56 ± 0.14x10−35 m2/sr) for the 1285 cm−1 mode of CO2 as the reference C 2016 Author(s) All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/) [http://dx.doi.org/10.1063/1.4942109] I INTRODUCTION The Raman spectra and cross sections of toxic gases are important for the detection of these gases using Raman spectroscopy in the fingerprint region 400-1400 cm−1 Raman spectra and cross sections are important for homeland security and other applications.1,2 Raman cross sections of a number of gases (CH4, C2H6, C3H8, C6H6, CO, CO2, F2, HBr, HCl, HF, H2, H2O, H2S, N2, NH3, ND3, NO, N2O, O2, O3, and SO2) have been reported previously.3–8 In this paper, we report the measurement of the Raman spectra and cross sections of ammonia (NH3), chlorine (Cl2), hydrogen sulfide (H2S), phosgene (CCl2O), and sulfur dioxide (SO2) toxic gases in the fingerprint region 400-1400 cm−1 using the Raman cross section of the 1285 cm−1 mode of carbon dioxide (CO2) as the reference.9 Raman cross sections of NH3, Cl2, H2S, and CClO2 have been measured for the first time in the fingerprint region Our value of the Raman cross section of SO2 is 1.5x larger than that reported previously.3,4 II EXPERIMENTAL Schematic of the optical setup of the Raman system is the same as reported previously.10,11 The 532 nm pump laser propagates in the horizontal direction (z-axis) through the flow cell The laser a Correspondence to R L Aggarwal, MIT Lincoln Laboratory, Lexington, MA 02420-9108, USA Email: aggarwal@ll.mit edu 2158-3226/2016/6(2)/025310/6 6, 025310-1 © Author(s) 2016 025310-2 Aggarwal et al AIP Advances 6, 025310 (2016) was polarized perpendicular to the direction of propagation (z-axis) The Raman signal is collected along the x-axis The magnification M of the image of the laser focal spot on the spectrometer slit is 1.6, which is the ratio of the 40 mm focal length focusing lens and the 25 mm focal length collection lens The diameter D of the laser focal spot, located in the center of the flow cell, was 50 µm There is small (

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