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Xiong Liu Harvard-Smithsonian Center for Astrophysics Kelly Chance, Thomas Kurosu, Christopher Sioris, Robert.

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Presentation on theme: "Xiong Liu Harvard-Smithsonian Center for Astrophysics Kelly Chance, Thomas Kurosu, Christopher Sioris, Robert."— Presentation transcript:

1 Xiong Liu (xliu@cfa.harvard.edu)xliu@cfa.harvard.edu Harvard-Smithsonian Center for Astrophysics Kelly Chance, Thomas Kurosu, Christopher Sioris, Robert Spurr, Randall Martin, Mike Newchurch SSAI, Lanham, Maryland April 11, 2006 Ozone Profile and Tropospheric Ozone Retrievals from GOME

2 2 Outline n Introduction n Examples of Retrievals n Algorithm Description u Instrument Model u Forward Model u Inverse Model n Retrieval Characterization u Information Content u Error Analysis n Intercomparison with TOMS, Dobson/Brewer, SAGE, and Ozonesonde Measurements n Summary and Future Outlook

3 3 Introduction nSinger and Wentworth [1957] first proposed to derive stratospheric ozone profiles from backscattered UV radiation. nThe idea has been successfully applied by the BUV, SBUV, SBUV/2 instruments to derive a ~35-year record of ozone profiles. nHowever, SBUV-like instruments provide reliable ozone profile information mainly between 1-20 mb. Between 20 mb and surface, ozone profile could not be resolved, although column ozone amount is reliably derived (Bhartia et al., 1996). nCan we do better especially in the troposphere??? nChance et al. (1997) performed a theoretical study to demonstrate that ozone profiles including tropospheric ozone can be derived from UV/Visible spectra (e.g., GOME and SCIAMACHY).

4 4 Introduction nGOME: launched in April 1995, measures radiances in 240-790 nm with a moderate resolution of 0.2-0.4 nm and high SNR nFour physically-based ozone profile algorithms: u Munro et al., 1998: 264-307 nm & 326-335 nm (2-step, empirical corr.)  Hoogen et al., 1999: 290-355 nm (empirical Chebyshev poly.) u Hasekamp and Landgraf, 2001: 290-313 nm u van der A et al., 2002: 260-340 nm (empirical correction) u Indicates calibration problems and the importance of calibrations nTropospheric O 3 data have not yet been published from these algorithms. Three challenges to get good tropospheric ozone: u Consistent and accurate calibration u High fitting precision u 90% total ozone above nWe recently developed our own ozone profile algorithm for GOME data and demonstrated that valuable tropospheric ozone can be derived from GOME (Liu et al., 2005, 2006a, 2006b, in press, 2006c submitted to ACP).

5 5 Examples of Retrievals (Ozone Profile) Ozone hole Biomass burning over Indonesia

6 6 Examples of Tropospheric Column Ozone (TCO) Biomass burning over Indonesia Zonal contrast in the tropics

7 7 GOME Tropospheric Column Ozone (1996-1999)

8 8 Algorithm Description n Measurements: 289-307 nm, 325-340 nm, 368-372 nm, coadd 8 channel 2 pixels to channel 1 resolutions (960 x 80 km 2 ) n Results: u Partial Column O 3 at 11 layers (each ~5km thick except for the top layer) u Now at 24 layers (each ~2.5-km thick) u NCEP tropopause to separate stratosphere & troposphere (2-3/4-6 layers) n Spectral fitting + Optimal Estimation + LIDORT n Three Keys:  Accurate calibration of the measurements  Accurate forward modeling (LIDORT with additional corrections)  Good knowledge of climatological a priori information (mean and standard deviation) and measurement errors Liu et al., 2005, JGR

9 9 High Resolution Solar Reference Spectrum

10 10 Instrument Model n Use GDP extraction software with all standard corrections n Instrument slit function characterization (Chance, 1998) u Assume Gaussian, use non-linear least squares fitting u High resolution solar reference spectrum (Caspar and Chance, 1998) u Variable slit widths (21 spectral pixels in 5-pixel increments)

11 11 Instrument Model n Wavelength calibration (Caspar and Chance, 1997) u Similarly determined except with variable slit widths (15 spectral pixels in 3-pixel increments) u Include wavelength shifts among radiances, irradiances and trace gas cross sections in the spectral fitting.

12 12 Instrument Model n Undersampling correction (Chance, 1998) u GOME significantly undersamples the spectrum u Use the high-resolution solar spectrum to simulate the sampling process and determine two basis functions for undersampling correction u Include a scaling factor for each basis function in the fitting n Radiometric Calibration and Degradation Correction u Wavelength-dependent bias in Channel 1 (van der A et al, 2002) u Degradation in reflectance since 1998 due to the build-up of a thin ice layer on scan mirror (Tanzi et al., 2001) u Include a wavelength-dependent correction (2 nd -order polynomial) in the fitting in 289-307 nm, constrained by the total ozone derived from the Huggins bands and the a priori profiles. u Degradation since 2000 largely affects the retrieved tropospheric ozone u External degradation correction is necessary. u Degradation correction derived using ozone profile climatology or observations [van der A et al., 2002; Landgraf et al., 2005] shows significant variation with latitude and station.

13 13 Instrument Model Liu et al., 2006, submitted to ACP n We derive an simpler scheme by comparing global-averaged reflectance over 60ºN- 60ºS to that in the first six months with additional steps to remove SZA and seasonal dependent components. n Degradation largely depends on scan-angle and wavelength.

14 14 Forward Model n LIDORT with pseudo-spherical approximation and 6 streams n Polarization correction with a look-up table: wavelength, total ozone, surface albedo and pressure, viewing geometry (courtesy of Roeland F. van Oss) n Ring effect: directly model the 1 st -oder RRS of the direct beam u Account for dependence on ozone profile and SZA (Sioris & Evans, 2002) u Use actual GOME solar irradiance u Ring spectra are updated when the total ozone change is > 20 DU u Scaling parameters are fitted in retrieval. n Clouds/Surface: Lambertian surface, Independent pixel approx. u Cloud-top pressure from GOMECAT (Kurosu et al., 1999) u Initial surface albedo from an albedo database (Koelemeijer et al., 2003) u Cloud fraction is derived from 370 nm and fixed by assuming a cloud albedo of 80% unless it is overcast, when we derive cloud albedo. u Surface albedo is varied in the retrievals u A wavelength-dependent albedo (2 nd polynomial) is used for channel 2

15 15 Forward Model n Aerosols n Monthly mean SAGE-II stratospheric aerosols (extinction & effective radius) (Bauman et al., 2003) n Monthly mean GOCART tropospheric aerosols (dust, sulfate, black & organic carbon, coarse and fine sea salt) (Chin et al., 2002) as described in Martin et al. (2003), optical properties (using Mie ) are externally mixed. n Wavelength-dependent surface albedo accounts for residual aerosol effects. http://hyperion.gsfc.nasa.gov/People/Chin/aot.html

16 16 Forward Model n Trace Gases: u Only O 3 is modeled in LIDORT with ozone cross sections by Daumont et al. (1992), Brion et al. (1993), Malicet et al. (1995) u Previous version: fit cross sections of NO 2, SO 2, BrO u Now fit weighting functions of NO 2, SO 2, BrO, and HCHO weighted by profile shapes from models due to large AMF variation with wavelength  NO 2 : PRATMO + GEOS-CHEM  BrO: PRATMO + well mixed in the troposphere  SO 2 /HCHO: GEOS-CHEM model simulations, no stratospheric n NCEP surface & tropopause pressure, ECMWF temperature n Effective viewing geometry (integrate and average geometric path lengths from west to east edge) n Weighting functions other than ozone, albedo, and shift parameters are derived with the finite difference approach.

17 17 Inverse Model n Measurement vector: n State vector: ozone variables + auxiliary parameters (albedo, shifts, trace gas, Ring effect, undersampling, degradation etc.) n Measurement error: GOME random-noise error (RSS of I + F, uncorrelated) n A priori information: n 3-D (month, latitude, altitude) ozone climatology by McPeters et al. [2003]: mean and standard deviations at 61 levels (0-60 km) (from 15 years of SAGE, ozonesonde and MLS) n Use a correlation length of 6 km to construct a priori covariance matrix n Other parameters: assumed empirically or based on retrieval statistics and are uncorrelated with the rest

18 18 Inverse Model n Convergence criteria: ozone/cost function change <1% n Convergence: 3-5 iterations, usually 2-3 iterations if initialized with a previous retrieval n One orbit: 36 mins on a 3.2-GHz processor (LIDORT, variable slit/wavelength calibrations), process 1-day GOME data in 8.7 hrs and process GOME-2 data daily with 3 such CPUs n Fitting residuals:

19 19 Informational Analysis --- Averaging Kernels VR: 7-12 km (at 10-37 km) 7-12 km (at 7-37 km) 8-12 km (at 20-38 km)

20 20 Informational Analysis --- DFS and A Priori Influence DFS: 1.2 DFS in the tropics, 0.5 at high latitudes A Priori influence in TCO: 15% in the tropics, 50% at high-latitudes

21 21 Error Analysis Precision: 2-8% (< 2DU) in the strat., <12%(5DU) in the troposphere Smoothing: 40 km, and 30% at <10 km TO: <2 DU(0.5%); 3 DU (1.0%) SCO: <2 DU(1%); 2-5 DU (1-2%) TCO: 1.5-3 DU(6-10%); 3-6 DU(12-20%)

22 22 Error Analysis Liu et al., 2005, JGR

23 23 Total Column Ozone Comparison Liu et al., 2005, 2006a, 2006b (in press) n Comparisons with total ozone /ozonesonde at 33 sonde stations n TOMS: avg. points within GOME, mean biases are <6 DU (2%) at most stations with 1  <1.5% in tropics and <2.4% at high latitudes n Dobson: ±8hrs, ±1.5ºlat, ±500km lon, mean biases are mostly <5 DU (2%) with 1  < 3% in the tropics and <5% at high latitudes

24 24 Intercomparison with SAGE-II Liu et al., 2005, JGR; Liu et al., 2006, in press n Comparisons with SAGE-II in 1996-1999 down to ~15 km: same day, ±1.5ºlat, ±5ºlon n Apply GOME averaging kernels n Systematic biases: usually <15% with 1  <10% at ~20-60 km and <15% at ~15-20 km n Column ozone: negative biases of 3-6 DU at 35-60 km, <2.5 DU at ~15-35 km

25 25 Comparison with OzonesondeTropospheric Column Ozone

26 26 Comparison with Ozonesonde Tropospheric Column Ozone

27 27 Comparison with Ozonesonde Tropospheric Column Ozone n GOME tropospheric column ozone captures most of the temporal variability in ozonesonde TCO.

28 28 n Mean biases: <3.3 DU (15%) at 30 stations; 1  : 3-8 DU (12-27%) n Improvements over a priori at most stations: either reduces MBs or 1  or increases the correlation Comparison with Ozonesonde Tropospheric Column Ozone

29 29 Comparison with Ozonesonde and SAGE-II SCO n Stratospheric column ozone between layer 4 and 7 (15~35 km) or between tropopause and layer 7 n GOME/SONDE SCO (15-35 km): usually higher by 8-20 DU (5-8%) at CI & most tropical stations n GOME/SAGE-II SCO (~15-35 km): usually within ±2.5 DU (1.5%) except for 3 Northern European stations

30 30 Comparison with Ozonesonde SCO http://www.cmdl.noaa.gov/infodata/ftpdata.html n GOME SCO compares better with 1%-KI buffered than 2%-KI unbuffered by 11-16 DU. n Altitude-dependent total ozone normalization reduces the bias contrast and GOME/sonde biases mainly with 2%-KI unbuffered.

31 31 Profile Comparison with Ozonesonde n Systematic biases n Large positive biases of (30-70%) at Carbon Iodine and most tropical stations

32 32 Profile Comparison with Ozonesonde n The biases relative to 1%-buffered is usually smaller by 5-15%. n Altitude-dependent homogenization reduces the bias with 2%-unbuffered. n Uncorrected altitude hysteresis can account for 5-15% biases.

33 33 Profile Comparison with Ozonesonde and SAGE-II n GOME/SAGE-II: usually <5% at layer 5 and 8-20% for layer 4 n GOME/Sonde: mostly 5-20% for layer 5 and 20-60% for layer 4

34 34 Summary and Future Outlook nOzone profiles and tropospheric column ozone are retrieved from GOME spectra (289-307 nm, 325-340 nm) using the optimal estimation after extensive treatments of wavelength and radiometric calibrations and forward modeling. nRetrieved TO compares well with TOMS and Dobson/Brewer measurements to within 2% at most locations. nThe mean biases and 1  with SAGE are usually within 15% down to ~15 km. nThe retrieved TCO captures most of the temporal variability in ozonesonde TCO; the mean biases are usually within 15% and 1  are within 13-27%. nThe large biases between GOME and ozonesonde in the stratosphere and upper troposphere at carbon iodine stations and most stations in the tropics, reflect biases in ozone retrievals as well as ozonesonde measurements. nThe biases depend on sonde technique, sensor solution and data processing, therefore demonstrating the need to homogenize available ozonesonde datasets and standardize future operational procedures for reliable satellite validation. n Derive ozone profiles from GOME data during July 1995 to May 2003. n Continue to improve and speed up the retrievals and apply this algorithm to SCIMACHY, GOME-2, and OMI data.

35 35 Acknowledgements nSupported by NASA and the Smithsonian Institution nESA and DLR nTOMS, SAGE, WOUDC, SHADOZ, CMDL nNCEP, ECMWF, GEOS-CHEM, GOCART, PRATMO nG. Labow for providing ozone profile climatology.


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