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Atmospheric Measurement Techniques An interactive open-access journal of the European Geosciences Union
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© Author(s) 2019. This work is distributed under
the Creative Commons Attribution 4.0 License.
© Author(s) 2019. This work is distributed under
the Creative Commons Attribution 4.0 License.

Submitted as: research article 06 Jun 2019

Submitted as: research article | 06 Jun 2019

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This discussion paper is a preprint. A revision of the manuscript is under review for the journal Atmospheric Measurement Techniques (AMT).

The use of O2 1.27 µm absorption band revisited for GHG monitoring from space and application to MicroCarb

Jean-Loup Bertaux1,4, Alain Hauchecorne1, Franck Lefèvre1,6, François-Marie Breon5, Laurent Blanot3, Denis Jouglet2, Pierre Lafrique2, and Pavel Akaev4 Jean-Loup Bertaux et al.
  • 1LATMOS/IPSL, UVSQ Université Paris-Saclay, Sorbonne Université, CNRS, 11 Boulevard d’Alembert, 78280 Guyancourt, France
  • 2Centre National d’Etudes Spatiales, CST, 18 av.Edouard Belin, 31401 Toulouse, France
  • 3ACRI-ST, 11 Boulevard d’Alembert, 78280 Guyancourt, France
  • 4Laboratory for planetary and exoplanetary atmospheres, IKI/RAN, Moscow,Russia
  • 5LSCE, CEA/CNRS/ Université de Versailles Saint-Quentin, 91191 Gif-sur-Yvette, France
  • 6LATMOS/IPSL, Sorbonne Université, UVSQ, CNRS, Paris, France

Abstract. Monitoring CO2 from space is essential to characterize the spatio/temporal distribution of this major greenhouse gas, and quantify its sources and sinks. The mixing ratio of CO2 to dry air can be derived from the CO2/O2 column ratio. The O2 column is usually derived form its absorption signature on the solar reflected spectra over the O2 A-band (i.e. OCO-2, Tanso/Gosat, Tansat). As a result of atmospheric scattering, the atmospheric path length varies with the aerosols load, their vertical distribution, and their optical properties. The spectral distance between the O2 A-band (0.76 µm) and the CO2 absorption band (1.6 µm) results in significant uncertainties due to the varying spectral properties of the aerosols over the globe.

There is another O2 absorption band at 1.27 µm with weaker lines than in the A-band. As the wavelength is much nearer to the CO2 and CH4 bands, there is less uncertainty when using it as a proxy of the atmospheric path length to the CO2 and CH4 bands. This O2 band is used by the TCCON network implemented for the validation of space-based GHG observations. However, this absorption band is contaminated by the spontaneous emission of the excited molecule O2*, which is produced by the photo-dissociation of O3 molecules in the stratosphere and mesosphere. From a satellite looking nadir, this emission has a similar shape as the absorption signal that is used.

In the frame of the CNES MicroCarb project, scientific studies have been performed in 2016–2018 to explore the problems associated to this O2* airglow contamination and methods to correct it. A theoretical synthetic spectrum of the emission was derived from a new approach, based on A21 Einstein coefficients information contained in the line-by-line HITRAN 2016 data base. The shape of our synthetic spectrum is fully validated when compared to O2* airglow spectra observed by SCIAMACHY/ENVISAT in limb viewing.

We have designed an inversion scheme of SCIAMACHY limb viewing spectra, allowing to determine the vertical distribution of the Volume Emision Rate of the O2* airglow. The VER profiles and corresponding integrated nadir intensities were both compared to a model of the emission based on the chemical-transport model REPROBUS. The airglow intensities depend mostly on the Solar Zenith Angle (both in model and data) and the model underestimate the observed emission by ∼ 15 %. This is fully confirmed with SCIAMACHY nadir viewing measurements over the oceans: in such conditions, we have disentangled and retrieved the nadir O2* emission in spite of the moderate spectral resolving power (∼ 860). It is shown that with the MicroCarb spectral resolution power (25,000) and SNR, the contribution of the O2* emission at 1.27 µm to the observed spectral radiance in nadir viewing may be disentangled from the lower atmosphere/ground absorption signature with a great accuracy. Simulations with 4ARCTIC radiative transfer inversion tool have shown that the CO2 mixing ratio may be retrieved with the accuracy required for quantifying the CO2 natural sources and sinks (pressure level error ≤ 1 hPa, XCO2 accuracy better than 0.4 ppmv) with only the O2 1.27 µm band. As a result of these studies (at an intermediate phase), it was decided to include this band (B4) in the MicroCarb design, while keeping the O2 A band for reference (B1). Our approach is very similar (likely identical), to the approach of Sun et al. (2018) who also analysed the potential of the O2 1.27 µm band and concluded favourably for GHG monitoring from space. We advocate for the inclusion of this O2 band on other GHG monitoring future space missions, such as GOSAT-3 and EU/ESA CO2-M missions, for a better GHG retrieval.

Jean-Loup Bertaux et al.
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Status: final response (author comments only)
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Jean-Loup Bertaux et al.
Jean-Loup Bertaux et al.
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Publications Copernicus
Short summary
Monitoring of Green House Gases from space is usually done by measuring the quantity of CO2 and O2 in the atmosphere from their spectral absorption imprinted on the solar spectrum backscattered upwards. We show that the use of the near infrared band of O2 at 1.27 µm, instead of the O2 band at 0.76 nm used up to now, may be more appropriate to better account for aerosols, in spite of a known airglow emission from ozone. The climate space mission MicroCarb (launch in 2021) includes this new band.
Monitoring of Green House Gases from space is usually done by measuring the quantity of CO2 and...