Atmospheric Measurement Techniques (Jan 2021)
Intercomparison of MAX-DOAS vertical profile retrieval algorithms: studies on field data from the CINDI-2 campaign
- J.-L. Tirpitz,
- U. Frieß,
- F. Hendrick,
- C. Alberti,
- C. Alberti,
- M. Allaart,
- A. Apituley,
- A. Bais,
- S. Beirle,
- S. Berkhout,
- K. Bognar,
- T. Bösch,
- I. Bruchkouski,
- A. Cede,
- A. Cede,
- K. L. Chan,
- K. L. Chan,
- M. den Hoed,
- S. Donner,
- T. Drosoglou,
- C. Fayt,
- M. M. Friedrich,
- A. Frumau,
- L. Gast,
- C. Gielen,
- C. Gielen,
- L. Gomez-Martín,
- N. Hao,
- A. Hensen,
- B. Henzing,
- C. Hermans,
- J. Jin,
- K. Kreher,
- J. Kuhn,
- J. Kuhn,
- J. Lampel,
- J. Lampel,
- A. Li,
- C. Liu,
- H. Liu,
- J. Ma,
- A. Merlaud,
- E. Peters,
- E. Peters,
- G. Pinardi,
- A. Piters,
- U. Platt,
- U. Platt,
- O. Puentedura,
- A. Richter,
- S. Schmitt,
- E. Spinei,
- E. Spinei,
- D. Stein Zweers,
- K. Strong,
- D. Swart,
- F. Tack,
- M. Tiefengraber,
- M. Tiefengraber,
- R. van der Hoff,
- M. van Roozendael,
- T. Vlemmix,
- J. Vonk,
- T. Wagner,
- Y. Wang,
- Z. Wang,
- M. Wenig,
- M. Wiegner,
- F. Wittrock,
- P. Xie,
- C. Xing,
- J. Xu,
- M. Yela,
- C. Zhang,
- X. Zhao,
- X. Zhao
Affiliations
- J.-L. Tirpitz
- Institute of Environmental Physics, University of Heidelberg, Heidelberg, Germany
- U. Frieß
- Institute of Environmental Physics, University of Heidelberg, Heidelberg, Germany
- F. Hendrick
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- C. Alberti
- Meteorological Institute, Ludwig-Maximilians-Universität München, Munich, Germany
- C. Alberti
- now at: Institute of Meteorology and Climate Research (IMK-ASF), Karlsruhe Institute of Technology (KIT), Karlsruhe, Germany
- M. Allaart
- Royal Netherlands Meteorological Institute (KNMI), De Bilt, the Netherlands
- A. Apituley
- Royal Netherlands Meteorological Institute (KNMI), De Bilt, the Netherlands
- A. Bais
- Laboratory of Atmospheric Physics, Aristotle University of Thessaloniki, Thessaloniki, Greece
- S. Beirle
- Max Planck Institute for Chemistry, Mainz, Germany
- S. Berkhout
- National Institute for Public Health and the Environment (RIVM), Bilthoven, the Netherlands
- K. Bognar
- Department of Physics, University of Toronto, Toronto, Canada
- T. Bösch
- Institute for Environmental Physics, University of Bremen, Bremen, Germany
- I. Bruchkouski
- National Ozone Monitoring Research and Education Center (NOMREC), Belarusian State University, Minsk, Belarus
- A. Cede
- LuftBlick Earth Observation Technologies, Mutters, Austria
- A. Cede
- NASA-Goddard Space Flight Center, Greenbelt, MD, USA
- K. L. Chan
- Meteorological Institute, Ludwig-Maximilians-Universität München, Munich, Germany
- K. L. Chan
- now at: Remote Sensing Technology Institute (IMF), German Aerospace Center (DLR), Oberpfaffenhofen, Germany
- M. den Hoed
- Royal Netherlands Meteorological Institute (KNMI), De Bilt, the Netherlands
- S. Donner
- Max Planck Institute for Chemistry, Mainz, Germany
- T. Drosoglou
- Laboratory of Atmospheric Physics, Aristotle University of Thessaloniki, Thessaloniki, Greece
- C. Fayt
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- M. M. Friedrich
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- A. Frumau
- Netherlands Organisation for Applied Scientific Research (TNO), Utrecht, the Netherlands
- L. Gast
- National Institute for Public Health and the Environment (RIVM), Bilthoven, the Netherlands
- C. Gielen
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- C. Gielen
- now at: Institute for Astronomy, KU Leuven, Leuven, Belgium
- L. Gomez-Martín
- National Institute of Aerospatial Technology (INTA), Madrid, Spain
- N. Hao
- Remote Sensing Technology Institute, German Aerospace Center (DLR), Oberpfaffenhofen, Germany
- A. Hensen
- Netherlands Organisation for Applied Scientific Research (TNO), Utrecht, the Netherlands
- B. Henzing
- Netherlands Organisation for Applied Scientific Research (TNO), Utrecht, the Netherlands
- C. Hermans
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- J. Jin
- Meteorological Observation Centre, China Meteorological Administration, Beijing, China
- K. Kreher
- BK Scientific GmbH, Mainz, Germany
- J. Kuhn
- Institute of Environmental Physics, University of Heidelberg, Heidelberg, Germany
- J. Kuhn
- Max Planck Institute for Chemistry, Mainz, Germany
- J. Lampel
- Institute of Environmental Physics, University of Heidelberg, Heidelberg, Germany
- J. Lampel
- Airyx GmbH, Justus-von-Liebig-Straße 14, Eppelheim, Germany
- A. Li
- Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei, China
- C. Liu
- School of Earth and Space Sciences, University of Science and Technology of China, Hefei, China
- H. Liu
- School of Earth and Space Sciences, University of Science and Technology of China, Hefei, China
- J. Ma
- Chinese Academy of Meteorology Science, China Meteorological Administration, Beijing, China
- A. Merlaud
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- E. Peters
- Institute for Environmental Physics, University of Bremen, Bremen, Germany
- E. Peters
- now at: Institute for Protection of Maritime Infrastructures, Bremerhaven, Germany
- G. Pinardi
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- A. Piters
- Royal Netherlands Meteorological Institute (KNMI), De Bilt, the Netherlands
- U. Platt
- Institute of Environmental Physics, University of Heidelberg, Heidelberg, Germany
- U. Platt
- Max Planck Institute for Chemistry, Mainz, Germany
- O. Puentedura
- National Institute of Aerospatial Technology (INTA), Madrid, Spain
- A. Richter
- Institute for Environmental Physics, University of Bremen, Bremen, Germany
- S. Schmitt
- Institute of Environmental Physics, University of Heidelberg, Heidelberg, Germany
- E. Spinei
- NASA-Goddard Space Flight Center, Greenbelt, MD, USA
- E. Spinei
- now at: Virginia Polytechnic Institute and State University, Blacksburg, VA, USA
- D. Stein Zweers
- Royal Netherlands Meteorological Institute (KNMI), De Bilt, the Netherlands
- K. Strong
- Department of Physics, University of Toronto, Toronto, Canada
- D. Swart
- National Institute for Public Health and the Environment (RIVM), Bilthoven, the Netherlands
- F. Tack
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- M. Tiefengraber
- LuftBlick Earth Observation Technologies, Mutters, Austria
- M. Tiefengraber
- Department of Atmospheric and Cryospheric Sciences, University of Innsbruck, Innsbruck, Austria
- R. van der Hoff
- National Institute for Public Health and the Environment (RIVM), Bilthoven, the Netherlands
- M. van Roozendael
- Royal Belgian Institute for Space Aeronomy, Brussels, Belgium
- T. Vlemmix
- Royal Netherlands Meteorological Institute (KNMI), De Bilt, the Netherlands
- J. Vonk
- National Institute for Public Health and the Environment (RIVM), Bilthoven, the Netherlands
- T. Wagner
- Max Planck Institute for Chemistry, Mainz, Germany
- Y. Wang
- Max Planck Institute for Chemistry, Mainz, Germany
- Z. Wang
- Remote Sensing Technology Institute, German Aerospace Center (DLR), Oberpfaffenhofen, Germany
- M. Wenig
- Meteorological Institute, Ludwig-Maximilians-Universität München, Munich, Germany
- M. Wiegner
- Meteorological Institute, Ludwig-Maximilians-Universität München, Munich, Germany
- F. Wittrock
- Institute for Environmental Physics, University of Bremen, Bremen, Germany
- P. Xie
- Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei, China
- C. Xing
- School of Earth and Space Sciences, University of Science and Technology of China, Hefei, China
- J. Xu
- Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei, China
- M. Yela
- National Institute of Aerospatial Technology (INTA), Madrid, Spain
- C. Zhang
- School of Earth and Space Sciences, University of Science and Technology of China, Hefei, China
- X. Zhao
- Department of Physics, University of Toronto, Toronto, Canada
- X. Zhao
- now at: Air Quality Research Division, Environment and Climate Change Canada, Vancouver, Canada
- DOI
- https://doi.org/10.5194/amt-14-1-2021
- Journal volume & issue
-
Vol. 14
pp. 1 – 35
Abstract
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.