- KU Leuven Belgium
- National Institute for Aerospace Technology Spain
- University of Toronto Canada
- Max Planck Institute for Biophysical Chemistry Germany
- NASAs Goddard Space Flight Center, Greenbelt, MD, USA United States
- Belarusian State University Belarus
- Ludwig-Maximilians-Universität München Germany
- University of Toronto Canada
- University of Science and Technology of China China (People's Republic of)
- Karlsruhe Institute of Technology Germany
- University of Science and Technology of China China (People's Republic of)
- CHINESE ACADEMY OF METEOROLOGICAL SCIENCES China (People's Republic of)
- Chinese Academy of Sciences (中国科学院) China (People's Republic of)
- Royal Belgian Institute for Space Aeronomy Belgium
- National Institute for Public Health and the Environment Netherlands
- Chinese Academy of Sciences China (People's Republic of)
- Heidelberg University Germany
- Belarusian State University of Transport Belarus
- Chinese Academy of Meteorological Sciences China (People's Republic of)
- German Aerospace Center Germany
- Aristotle University of Thessaloniki Greece
- LUDWIG-MAXIMILIANS-UNIVERSITAET MUENCHEN Germany
- Chinese Academy of Science China (People's Republic of)
- Universität Innsbruck Austria
- Government of Canada Canada
- National Institute for Public Health and the Environment Netherlands
- Karlsruhe Institute of Technology Germany
- Royal Netherlands Meteorological Institute Netherlands
- METEOROLOGISK INSTITUTT Norway
- KU Leuven Belgium
- Netherlands Organisation for Applied Scientific Research Netherlands
- Anhui Institute of Optics and Fine Mechanics China (People's Republic of)
- Chinese Academy of Science (中国科学院) China (People's Republic of)
- National Institute for Public Health and the Environment Netherlands
- Max Planck Institute for Chemistry Germany
- SCIENCE AND TECHNOLOGY BV Netherlands
- Karlsruhe Institute of Technology (KIT) Germany
- Netherlands Organization for Scientific Research Netherlands
- Max Planck Society Germany
- KU Leuven Belgium
- Chinese Academy of Sciences, Shanghai Institute of Optics and Fine Mechanics China (People's Republic of)
- AIRYX GMBH Germany
- Environment and Climate Change Canada Canada
- University of Bremen Germany
- Ludwig-Maximilians-Universität München Germany
- Max Planck Institute for Heart and Lung Research Germany
- BK SCIENTIFIC GMBH Germany
- Max Plank Institute for Chemistry (MPIC), Mainz, Germany Germany
- Netherlands Organisation for Scientific Research Netherlands
The second Cabauw Intercomparison of Nitrogen Dioxide measuring Instruments (CINDI-2) took place in Cabauw (the Netherlands) in September 2016 with the aim of assessing the consistency of multi-axis differential optical absorption spectroscopy (MAX-DOAS) measurements of tropospheric species (NO2, HCHO, O3, HONO, CHOCHO and O4). This was achieved through the coordinated operation of 36 spectrometers operated by 24 groups from all over the world, together with a wide range of supporting reference observations (in situ analysers, balloon sondes, lidars, long-path DOAS, direct-sun DOAS, Sun photometer and meteorological instruments). In the presented study, the retrieved CINDI-2 MAX-DOAS trace gas (NO2, HCHO) and aerosol vertical profiles of 15 participating groups using different inversion algorithms are compared and validated against the colocated supporting observations, with the focus on aerosol optical thicknesses (AOTs), trace gas vertical column densities (VCDs) and trace gas surface concentrations. The algorithms are based on three different techniques: six use the optimal estimation method, two use a parameterized approach and one algorithm relies on simplified radiative transport assumptions and analytical calculations. To assess the agreement among the inversion algorithms independent of inconsistencies in the trace gas slant column density acquisition, participants applied their inversion to a common set of slant columns. Further, important settings like the retrieval grid, profiles of O3, temperature and pressure as well as aerosol optical properties and a priori assumptions (for optimal estimation algorithms) have been prescribed to reduce possible sources of discrepancies. The profiling results were found to be in good qualitative agreement: most participants obtained the same features in the retrieved vertical trace gas and aerosol distributions; however, these are sometimes at different altitudes and of different magnitudes. Under clear-sky conditions, the root-mean-square differences (RMSDs) among the results of individual participants are in the range of 0.01–0.1 for AOTs, (1.5–15) ×1014molec.cm-2 for trace gas (NO2, HCHO) VCDs and (0.3–8)×1010molec.cm-3 for trace gas surface concentrations. These values compare to approximate average optical thicknesses of 0.3, trace gas vertical columns of 90×1014molec.cm-2 and trace gas surface concentrations of 11×1010molec.cm-3 observed over the campaign period. The discrepancies originate from differences in the applied techniques, the exact implementation of the algorithms and the user-defined settings that were not prescribed. For the comparison against supporting observations, the RMSDs increase to a range of 0.02–0.2 against AOTs from the Sun photometer, (11–55)×1014molec.cm-2 against trace gas VCDs from direct-sun DOAS observations and (0.8–9)×1010molec.cm-3 against surface concentrations from the long-path DOAS instrument. This increase in RMSDs is most likely caused by uncertainties in the supporting data, spatiotemporal mismatch among the observations and simplified assumptions particularly on aerosol optical properties made for the MAX-DOAS retrieval. As a side investigation, the comparison was repeated with the participants retrieving profiles from their own differential slant column densities (dSCDs) acquired during the campaign. In this case, the consistency among the participants degrades by about 30 % for AOTs, by 180 % (40 %) for HCHO (NO2) VCDs and by 90 % (20 %) for HCHO (NO2) surface concentrations. In former publications and also during this comparison study, it was found that MAX-DOAS vertically integrated aerosol extinction coefficient profiles systematically underestimate the AOT observed by the Sun photometer. For the first time, it is quantitatively shown that for optimal estimation algorithms this can be largely explained and compensated by considering biases arising from the reduced sensitivity of MAX-DOAS observations to higher altitudes and associated a priori assumptions.