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Frequency Comb-referenced Measurements of Self- and Nitrogen-broadening in the m1 + m3 Band of Acetylene
We report measurements of self- and nitrogen-pressure broadening of the P(11) line in the ?{sub 1} + ?{sub 3} combination band of acetylene at 195 739.649 5135(80) GHz by absorption of radiation emitted by an extended cavity diode laser referenced to a femtosecond frequency comb. Broadening, shift a...
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Published in: | Journal of molecular spectroscopy 2011-03, Vol.266 (1) |
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container_title | Journal of molecular spectroscopy |
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creator | McRaven, C.P. Cich, M.J. Lopez, G.V. Sears, T.J. Hurtmans, D. Mantz, A.W. |
description | We report measurements of self- and nitrogen-pressure broadening of the P(11) line in the ?{sub 1} + ?{sub 3} combination band of acetylene at 195 739.649 5135(80) GHz by absorption of radiation emitted by an extended cavity diode laser referenced to a femtosecond frequency comb. Broadening, shift and narrowing parameters were determined at 296 K. For the most appropriate, hard collision, model in units of cm{sup -1}/atm, we find 0.146317(27), 0.047271(104) and -0.0070819(22) for the acetylene self-broadening, narrowing and shift, and 0.081129(35), 0.022940(74) and -0.0088913(25) respectively, for the nitrogen-broadening parameters. The uncertainties are expressed as one standard deviation (in parenthesis) in units of the last digit reported. These parameters are 2-3 orders of magnitude more precise than those reported in previous measurements. Similar analyses of the experimental data using soft collision and simple Voigt lineshape models were made for comparison. |
doi_str_mv | 10.1016/j.jms.2011.02.016 |
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Broadening, shift and narrowing parameters were determined at 296 K. For the most appropriate, hard collision, model in units of cm{sup -1}/atm, we find 0.146317(27), 0.047271(104) and -0.0070819(22) for the acetylene self-broadening, narrowing and shift, and 0.081129(35), 0.022940(74) and -0.0088913(25) respectively, for the nitrogen-broadening parameters. The uncertainties are expressed as one standard deviation (in parenthesis) in units of the last digit reported. These parameters are 2-3 orders of magnitude more precise than those reported in previous measurements. 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Broadening, shift and narrowing parameters were determined at 296 K. For the most appropriate, hard collision, model in units of cm{sup -1}/atm, we find 0.146317(27), 0.047271(104) and -0.0070819(22) for the acetylene self-broadening, narrowing and shift, and 0.081129(35), 0.022940(74) and -0.0088913(25) respectively, for the nitrogen-broadening parameters. The uncertainties are expressed as one standard deviation (in parenthesis) in units of the last digit reported. These parameters are 2-3 orders of magnitude more precise than those reported in previous measurements. 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Broadening, shift and narrowing parameters were determined at 296 K. For the most appropriate, hard collision, model in units of cm{sup -1}/atm, we find 0.146317(27), 0.047271(104) and -0.0070819(22) for the acetylene self-broadening, narrowing and shift, and 0.081129(35), 0.022940(74) and -0.0088913(25) respectively, for the nitrogen-broadening parameters. The uncertainties are expressed as one standard deviation (in parenthesis) in units of the last digit reported. These parameters are 2-3 orders of magnitude more precise than those reported in previous measurements. Similar analyses of the experimental data using soft collision and simple Voigt lineshape models were made for comparison.</abstract><cop>United States</cop><doi>10.1016/j.jms.2011.02.016</doi></addata></record> |
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subjects | ABSORPTION ACETYLENE ATOMIC AND MOLECULAR PHYSICS frequency comb LASERS pressure broadening RADIATIONS |
title | Frequency Comb-referenced Measurements of Self- and Nitrogen-broadening in the m1 + m3 Band of Acetylene |
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