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Vibrational-vibrational and vibrational-thermal energy transfers of CO2 with N2 from MIPAS high-resolution limb spectra

We present a retrieval of several vibrational‐vibrational (V V) and vibrational‐thermal (V‐T) collisional rate coefficients affecting the populations of the CO2 levels emitting at 10, 4.3 and 2.7 μm from high‐resolution limb atmospheric spectra taken by Michelson Interferometer for Passive Atmospher...

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Published in:Journal of geophysical research. Atmospheres 2015-08, Vol.120 (15), p.8002-8022
Main Authors: Jurado-Navarro, Á. A., López-Puertas, M., Funke, B., García-Comas, M., Gardini, A., Stiller, G. P., Clarmann, T. von
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container_issue 15
container_start_page 8002
container_title Journal of geophysical research. Atmospheres
container_volume 120
creator Jurado-Navarro, Á. A.
López-Puertas, M.
Funke, B.
García-Comas, M.
Gardini, A.
Stiller, G. P.
Clarmann, T. von
description We present a retrieval of several vibrational‐vibrational (V V) and vibrational‐thermal (V‐T) collisional rate coefficients affecting the populations of the CO2 levels emitting at 10, 4.3 and 2.7 μm from high‐resolution limb atmospheric spectra taken by Michelson Interferometer for Passive Atmospheric Sounding (MIPAS). This instrument has a high spectral resolution (0.0625 cm−1) and a wide spectral coverage (from 685 to 2410 cm−1) that allow measuring and discriminating among the many bands originating the atmospheric 4.3 μm radiance. Also its high sensitivity allows measuring the atmospheric limb emission in a wide altitude range, from 20 to 170 km in its middle and upper atmosphere modes, and hence obtain information on the temperature dependence of the collisional rates. In particular, we retrieve the rate coefficients and their temperature dependence in the 130–250 K range of the following processes: CO2(vd,v3)+N2⇌CO2(vd,v3−1)+N2(1) with vd=2v1+v2=2,3, and 4; CO2(v1,v2,l,1,r)+M⇌CO2(v1′,v2′,l′,1,r′)+M with Δvd=vd′−vd=0 and Δl = 0; and with Δvd=0 and Δl ≠ 0. In addition we have also retrieved the thermal relaxation of CO2(v3) into the v1 and v2 modes, e.g., CO2(vd,v3)+M⇌CO2(vd′,v3−1)+M with Δvd=2–4 and Δv3=−1 and the efficiency of the excitation of N2(1) by O(1D). All of them were retrieved with a much better accuracy than were known before. The new rates have very important effects on the atmospheric limb radiance in the 10, 4.3 and 2.7 μm spectral regions (5–8% at 4.3 μm) and allow a more accurate inversion of the CO2 volume mixing ratio in the mesosphere and lower thermosphere from measurements taken in those spectral regions. Key Points Crucial V‐V and V‐T rates controlling CO2 IR emission have been retrieved These rates are very different from current values and are much more accurate They are important for CO2 measurements in the mesosphere and lower thermosphere
doi_str_mv 10.1002/2015JD023429
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A. ; López-Puertas, M. ; Funke, B. ; García-Comas, M. ; Gardini, A. ; Stiller, G. P. ; Clarmann, T. von</creator><creatorcontrib>Jurado-Navarro, Á. A. ; López-Puertas, M. ; Funke, B. ; García-Comas, M. ; Gardini, A. ; Stiller, G. P. ; Clarmann, T. von</creatorcontrib><description>We present a retrieval of several vibrational‐vibrational (V V) and vibrational‐thermal (V‐T) collisional rate coefficients affecting the populations of the CO2 levels emitting at 10, 4.3 and 2.7 μm from high‐resolution limb atmospheric spectra taken by Michelson Interferometer for Passive Atmospheric Sounding (MIPAS). This instrument has a high spectral resolution (0.0625 cm−1) and a wide spectral coverage (from 685 to 2410 cm−1) that allow measuring and discriminating among the many bands originating the atmospheric 4.3 μm radiance. Also its high sensitivity allows measuring the atmospheric limb emission in a wide altitude range, from 20 to 170 km in its middle and upper atmosphere modes, and hence obtain information on the temperature dependence of the collisional rates. In particular, we retrieve the rate coefficients and their temperature dependence in the 130–250 K range of the following processes: CO2(vd,v3)+N2⇌CO2(vd,v3−1)+N2(1) with vd=2v1+v2=2,3, and 4; CO2(v1,v2,l,1,r)+M⇌CO2(v1′,v2′,l′,1,r′)+M with Δvd=vd′−vd=0 and Δl = 0; and with Δvd=0 and Δl ≠ 0. In addition we have also retrieved the thermal relaxation of CO2(v3) into the v1 and v2 modes, e.g., CO2(vd,v3)+M⇌CO2(vd′,v3−1)+M with Δvd=2–4 and Δv3=−1 and the efficiency of the excitation of N2(1) by O(1D). All of them were retrieved with a much better accuracy than were known before. The new rates have very important effects on the atmospheric limb radiance in the 10, 4.3 and 2.7 μm spectral regions (5–8% at 4.3 μm) and allow a more accurate inversion of the CO2 volume mixing ratio in the mesosphere and lower thermosphere from measurements taken in those spectral regions. 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P.</creatorcontrib><creatorcontrib>Clarmann, T. von</creatorcontrib><title>Vibrational-vibrational and vibrational-thermal energy transfers of CO2 with N2 from MIPAS high-resolution limb spectra</title><title>Journal of geophysical research. Atmospheres</title><addtitle>J. Geophys. Res. Atmos</addtitle><description>We present a retrieval of several vibrational‐vibrational (V V) and vibrational‐thermal (V‐T) collisional rate coefficients affecting the populations of the CO2 levels emitting at 10, 4.3 and 2.7 μm from high‐resolution limb atmospheric spectra taken by Michelson Interferometer for Passive Atmospheric Sounding (MIPAS). This instrument has a high spectral resolution (0.0625 cm−1) and a wide spectral coverage (from 685 to 2410 cm−1) that allow measuring and discriminating among the many bands originating the atmospheric 4.3 μm radiance. Also its high sensitivity allows measuring the atmospheric limb emission in a wide altitude range, from 20 to 170 km in its middle and upper atmosphere modes, and hence obtain information on the temperature dependence of the collisional rates. In particular, we retrieve the rate coefficients and their temperature dependence in the 130–250 K range of the following processes: CO2(vd,v3)+N2⇌CO2(vd,v3−1)+N2(1) with vd=2v1+v2=2,3, and 4; CO2(v1,v2,l,1,r)+M⇌CO2(v1′,v2′,l′,1,r′)+M with Δvd=vd′−vd=0 and Δl = 0; and with Δvd=0 and Δl ≠ 0. In addition we have also retrieved the thermal relaxation of CO2(v3) into the v1 and v2 modes, e.g., CO2(vd,v3)+M⇌CO2(vd′,v3−1)+M with Δvd=2–4 and Δv3=−1 and the efficiency of the excitation of N2(1) by O(1D). All of them were retrieved with a much better accuracy than were known before. The new rates have very important effects on the atmospheric limb radiance in the 10, 4.3 and 2.7 μm spectral regions (5–8% at 4.3 μm) and allow a more accurate inversion of the CO2 volume mixing ratio in the mesosphere and lower thermosphere from measurements taken in those spectral regions. 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Atmos</addtitle><date>2015-08-16</date><risdate>2015</risdate><volume>120</volume><issue>15</issue><spage>8002</spage><epage>8022</epage><pages>8002-8022</pages><issn>2169-897X</issn><eissn>2169-8996</eissn><abstract>We present a retrieval of several vibrational‐vibrational (V V) and vibrational‐thermal (V‐T) collisional rate coefficients affecting the populations of the CO2 levels emitting at 10, 4.3 and 2.7 μm from high‐resolution limb atmospheric spectra taken by Michelson Interferometer for Passive Atmospheric Sounding (MIPAS). This instrument has a high spectral resolution (0.0625 cm−1) and a wide spectral coverage (from 685 to 2410 cm−1) that allow measuring and discriminating among the many bands originating the atmospheric 4.3 μm radiance. Also its high sensitivity allows measuring the atmospheric limb emission in a wide altitude range, from 20 to 170 km in its middle and upper atmosphere modes, and hence obtain information on the temperature dependence of the collisional rates. In particular, we retrieve the rate coefficients and their temperature dependence in the 130–250 K range of the following processes: CO2(vd,v3)+N2⇌CO2(vd,v3−1)+N2(1) with vd=2v1+v2=2,3, and 4; CO2(v1,v2,l,1,r)+M⇌CO2(v1′,v2′,l′,1,r′)+M with Δvd=vd′−vd=0 and Δl = 0; and with Δvd=0 and Δl ≠ 0. In addition we have also retrieved the thermal relaxation of CO2(v3) into the v1 and v2 modes, e.g., CO2(vd,v3)+M⇌CO2(vd′,v3−1)+M with Δvd=2–4 and Δv3=−1 and the efficiency of the excitation of N2(1) by O(1D). All of them were retrieved with a much better accuracy than were known before. The new rates have very important effects on the atmospheric limb radiance in the 10, 4.3 and 2.7 μm spectral regions (5–8% at 4.3 μm) and allow a more accurate inversion of the CO2 volume mixing ratio in the mesosphere and lower thermosphere from measurements taken in those spectral regions. Key Points Crucial V‐V and V‐T rates controlling CO2 IR emission have been retrieved These rates are very different from current values and are much more accurate They are important for CO2 measurements in the mesosphere and lower thermosphere</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1002/2015JD023429</doi><tpages>21</tpages></addata></record>
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identifier ISSN: 2169-897X
ispartof Journal of geophysical research. Atmospheres, 2015-08, Vol.120 (15), p.8002-8022
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2169-8996
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source Wiley; Alma/SFX Local Collection
subjects Atmospheric sounding
Carbon dioxide
CO2
CO2, N2
Coefficients
Emission measurements
Geophysics
high-resolution IR spectra
Interferometers
Lower thermosphere
Mesosphere
Meteorology
MIPAS
Mixing ratio
non-LTE infrared emissions
Radiance
Regions
Resolution
Spectra
Spectral resolution
Spectrum analysis
Temperature
Temperature dependence
Thermal energy
Thermal relaxation
Thermosphere
Upper atmosphere
V-V and V-T rate coefficients
title Vibrational-vibrational and vibrational-thermal energy transfers of CO2 with N2 from MIPAS high-resolution limb spectra
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