National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 1 Atmospheric Infrared.

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National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 1 Atmospheric Infrared Sounder Validation of AIRS Retrievals of CO 2 via Comparison to In Situ Measurements Edward T. Olsen, Moustafa T. Chahine Luke L. Chen, Xun Jiang, Thomas S. Pagano & Yuk L. Yung Jet Propulsion Laboratory, California Institute of Technology Pasadena, California AGU 2008 Fall Meeting San Francisco CA Dec 15-19, 2008

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 2 Atmospheric Infrared Sounder  AIRS on Aqua: present  Expected to continue operation to 2011 and beyond  Background: spectrum, weighting functions, initialization  Comparison with Aircraft and FTIR Measurements  Matsueda (CONTRAIL) JAL flask measurements  Park Falls, WI FTIR  Bremen, GDR  Spitsbergen, Norway  AIRS Retrievals over additional FTIR Sites  Darwin, AU  Lauder, NZ Overview

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 3 Atmospheric Infrared Sounder Typical AIRS Infrared Spectrum AIRS Channels for Tropical Atmosphere with T_surf = 301K 2378 channels -  Δ  =  m band

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 4 Atmospheric Infrared Sounder AIRS sensitivity for retrieving CO 2 profiles AIRS is capable of retrieving CO 2 in 3 layers Mid-troposphere (Completed) 2002 to present Accuracy of ppmv Stratosphere (2009) Near-Surface (2010)

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 5 Atmospheric Infrared Sounder Our VPD CO 2 retrieval errors are also independent thus retrievals can be averaged to reduce the RMS errors. The VPD CO2 retrieval is a post processing step yielding a unique solution: It ingests the AIRS Level 2 products (T, H2O, O3) It assumes the same initial constant CO2 profile used in the Level 2 retrieval algorithm for consistency Independence of CO 2 solution with respect to the initial guess Our tests have demonstrated independence of the solution to assumed initial CO 2 over the range: 330 ppmv to 390 ppmv

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 6 Atmospheric Infrared Sounder  Aircraft CO 2 Profiles  Closest we can come to a true validation of AIRS CO 2 retrievals  Sparse dataset, especially for profiles reaching up to 12 km altitude  CONTRAIL (Matsueda) Flask Measurements  Affords long-term, seasonal and interannual comparison 30S to 30N  Narrow range of altitude: 11 km ± 1 km  Over ocean  TCCON FTIR Sites  Continuous daily observations  No nighttime, thus long gaps for high latitude sites during polar winter Available in situ measurements for validation and comparison

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 7 Atmospheric Infrared Sounder Aircraft data from Stephanie Vay (LaRC) INTEX-NA July 10-15, 2004 SPURT April 25-30, 2003 Comparison of Collocated V1.5x AIRS CO 2 (N_coll≥9) with INTEX-NA and SPURT Aircraft data from Peter Hoor et al.

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 8 Atmospheric Infrared Sounder Comparison of V1.5x AIRS CO 2 in 10°x10° Areas and CONTRAIL (Matsueda) Airborne Flask Measurements (flying at 10 km to 12 km altitude in 10° latitude zones) JAL Flights ~ two week intervals 30S ≤ LAT ≤ 33N 135E ≤ LON ≤ 152E 7-day averages of AIRS retrievals: LAT= +25° ± 5° LON = 143° ± 5° CONTRAIL individual flask measurements: LAT = +25° ± 5° 7-day averages of AIRS retrievals: LAT= -25° ± 5° LON = 150° ± 5° CONTRAIL individual flask measurements: LAT = -25° ± 5°

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 9 Atmospheric Infrared Sounder Park Falls FTS (Paul Wennberg) – Lat: N Lon: W – clear sky observations AIRS – Within 250km radius of Park Falls – clear & cloudy observations Vegetation uptake during growing season – 6->7 ppmv departure in June 2004/2005 Washenfelder. R. A., et al. (2006), J.Geophys. Res. 111, D22305, doi: /2006JD Monthly Averages Comparison of V1.5x AIRS CO 2 to Park Falls, WI Fourier Transform Spectrometer

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 10 Atmospheric Infrared Sounder Bremen FTIR data provided by Prof. Dr. Justus Notholt, University of Bremen Comparison of V1.5x AIRS CO 2 seasonal cycle and trend to Bremen FTIR (53.1N; 8.9E)

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 11 Atmospheric Infrared Sounder Spitsbergen FTIR data provided by Prof. Dr. Justus Notholt, University of Bremen Comparison of V1.5x AIRS CO 2 seasonal cycle and trend with Spitsbergen(78.9N; 12.4E)

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 12 Atmospheric Infrared Sounder  We have carried out comparisons with independent measurements between 30°S and 80°N  Excellent agreement with aircraft and FTIR as a function of season and latitude  TCCON network provides opportunity for frequent comparison of AIRS mid-tropospheric CO 2 retrievals with high-quality measurements of Column CO 2  Combined observations offer possibility of tracking the large- scale variation of CO 2 in the boundary layer  AIRS allows monitoring of distribution of global CO 2 in the free troposphere on a weekly basis  Good time and space coverage are important because significant spatiotemporal variability is apparent and appears to be strongly influenced by large-scale circulations such as the middle-latitude jet streams and synoptic weather systems Summary and Conclusions

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 13 Atmospheric Infrared Sounder AIRS V2.0 CO 2 monthly average, gridded data – Time Period: Sept 2002 through Dec 2004 – Global Coverage: 60°S to 90°N – Geospatial Resolution: 2° x 2.5° (lat x lon) – Averaged in time for each calendar month Access at the GES DISC – – ftp://acdisc.gsfc.nasa.gov/data/s4pa/Aqua_AIRS_Level3/AIRX3C2M.005 – M_V005&MetadataView=Brief – Data Format HDF-EOS Grid – Questions? Contact Pre-Release of Version 2.0 CO 2

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 14 Atmospheric Infrared Sounder BACKUP

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 15 Atmospheric Infrared Sounder AIRS AMSU-HSB Scan Patterns See Box on page 915 Bul. Am. Met. Soc June 2006 “There no such thing as cloud-free...It is just cirrus” GEWEX-ISCCP

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 16 Atmospheric Infrared Sounder AIRS Sensitivity Function for mid-Tropospheric CO 2 Average weighting function for 13 selected CO 2 channels in 15  m band Peak sensitivity occurs at 450 hPa (6.2 km) Width at half-maximum spans 700 hPa (3 km) to 200 hPa (12 km) Sensitivity to surface emission limited to less than 0.05 K radiance contribution

National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology Pasadena, California 17 Atmospheric Infrared Sounder AIRS mid-Tropospheric CO 2 Sensitivity Function for tropical, mid-latitude and polar regions Average weighting function for 13 selected CO 2 channels in 15  m band