New PoLArization ALgorithm

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Presentation transcript:

New PoLArization ALgorithm P. Liebing, IUP Bremen, SQWG PM4 New PoLArization ALgorithm SQWG PM4 Sep 2015 P. Liebing, IUP Bremen

Outline Suggestions for changes to polarization algorithm Suggestions for changes to polarization correction Some more things that need discussion Update on V9.02 P. Liebing, IUP Bremen, SQWG PM4

New Algorithm: General Synchronize and integrate 40 Hz PMD data TN: find relevant wavelength/pixel #, calculate effective delay, apply to 40Hz PMD data synchronized to BCPS Filter for spikes (Limb) Algorithm in TN, though, if someone has a better idea? Mirror model calibration of virtual sum and PMD signal NOTE: Bad pixels in VS, see below! Correct unpolarized ratio for cluster coverage Correct unpolarized ratio with unpolarized scale factor (no more SMR IB!) Data as ASCII file, monthly for nadir, yearly for limb Linear interpolation between data points? Compute average mi(PMD,DET) (IT dependent!) Algorithm in TN Use PMD 4 and 7 iteratively P. Liebing, IUP Bremen, SQWG PM4

New Algorithm: Other PMDs, Nadir Retrieve q,u from RTM LUT, calculate RTM polarization angle LUTs in form of SCIATRAN data (ASCII) f(month, RO #) Interpolation between geometrical points necessary NOTE: Optimized for IT=0.25s, larger no problem, smaller? Might require change of loops over ITs! Compute polarization sensitivity TN If glint: use RTM value for u directly Use PMD4/7 to detect glint (TN) Else if sensitivity≥0.2: Apply polarization angle algorithm P. Liebing, IUP Bremen, SQWG PM4

New Algorithm: Other PMDs, Nadir Else: use u(R) model: Use u(R) and calibrated reflectance Reflectance as average around fixed wavelengths (TN) Apply (possibly cos(q) dependent) parameterization u(R) TN, data as LUT Several options, not yet clear which method/data are going to be used Derive q with u(R) TN P. Liebing, IUP Bremen, SQWG PM4

New Algorithm: Other PMDs, Limb u(R) model everywhere: Use u(RTM) and calibrated reflectance LUTs in form of SCIATRAN data (ASCII) f(month, lat) Interpolation between geometrical points (TH, SZA, AZ) necessary Reflectance as average around fixed wavelengths (TN) u(R) parametrization (cos(q), TH, R) LUTs as ASCII, some fudging of geometry and reflectance necessary (limits) Derive q with u(R) TN P. Liebing, IUP Bremen, SQWG PM4

New Algorithm: Other PMDs, Limb Algorithm should be applied iteratively using polarization corrected reflectance (?) Option: Use effective MMEs from in-flight fits rather than V9 key data Above TH=Z1: Use q(R), u(R) directly(at least PMD 5) Above TH=Z2: use last values (even and odd TH steps separately) TH limits tbd Further option: TH dependent correction to unpolarized scale factor Data as ASCII P. Liebing, IUP Bremen, SQWG PM4

Polarization Correction In principle as before Improve nadir UV parametrization (between ~300 and 370 nm) Use new GOME approach, i.e., parameters as f(O3 column and effective albedo) Needs O3 columns from previous L2 RTM for albedo? UV correction for limb: Proposed algorithm in TN by Stefan Uses q(R),u(R) relationship – needs calibrated R for each pixel >= 260 nm Iterative approach (pol. corr.) Possibly use q(370nm), u(370nm) from LUT rather than PMD 1 P. Liebing, IUP Bremen, SQWG PM4

Things to do (IUP) Describe/document algorithm: started Provide IB scale factor f(a,t): needs to be redone for V9.02 Optimize Z1, Z2, TH corr. Provide SCIATRAN data for LUTs: can be delivered w/format description At least 2 different ones Rayleigh (over land) BRDF (v=7m/s, over ocean) (?) Thick ice cloud as lower limit Provide slopes for u(R) as tables or parameterization: Nadir: needs to be decided/done Limb: ready, only needs reformatting P. Liebing, IUP Bremen, SQWG PM4

Things to do (DLR) Implement algorithm Build SCIATRAN LUT and develop interpolation routines Optimize PMD synchronization (w/IUP) Limb: Spike filter (?) Read and apply all LUTs (u(R), TH corr.) Implement Gome-style polarization correction for Nadir UV Implement Limb UV correction: Needs additional LUTs (SCIATRAN, high-res.) P. Liebing, IUP Bremen, SQWG PM4

Things to Discuss Bad Pixel Mask! Old concept had smoothed or clipped M-Factors, new one (OBM M-Factors) doesn’t For Virtual sum we integrate over all wavelengths in PMD range, using interpolated (offset corrected) signal for bad pixels Calibrate: S(interpolated)*M1*M-Factor, where M_Factor≈±10000 …. Solution: Interpolate M-Factors over bad pixels, too That requires an adequate bad pixel detection Current BDPM not good enough for limb! I made my own, which is fixed in time (for ch. 6+) Includes the ones which have been masked by V8 BDPM For consistency, this should be used for Virtual sum and limb cloud algorithms P. Liebing, IUP Bremen, SQWG PM4

Things to Discuss Limb MMEs! There are still significant differences between V9 and fits to RTM Highly collinear data, even with 1 year integration Fits to RTM very model dependent Which are the correct MMEs? Check retrieved polarization For PMDs 1-3, polarization is ½ of expected with V9.00 (and mostly also V9.02, mind the time dependence) “Solution”: To apply effective MMEs from in-flight fits: For polarization correction, V9.02 KD have to be trusted P. Liebing, IUP Bremen, SQWG PM4

PMD 1 Effective MMEs vs. V9.02, Limb Effective PMD sensitivities vs. time (1 year average) Model: SCIATRAN (q,u)(R) m1 MPMD/MDET m2 m3 P. Liebing, IUP Bremen, SQWG PM4

PMD 2 Effective MMEs vs. V9.02, Limb Effective PMD sensitivities vs. time (1 year average) Model: SCIATRAN (q,u)(R) m1 MPMD/MDET m2 m3 P. Liebing, IUP Bremen, SQWG PM4

PMD 3 Effective MMEs vs. V9.02, Limb Effective PMD sensitivities vs. time (1 year average) Model: SCIATRAN (q,u)(R) m1 MPMD/MDET m2 m3 P. Liebing, IUP Bremen, SQWG PM4

PMD 4 Effective MMEs vs. V9.02, Limb Effective PMD sensitivities vs. time (1 year average) Model: SCIATRAN (q,u)(R) m1 MPMD/MDET m2 m3 P. Liebing, IUP Bremen, SQWG PM4

PMD 5 Effective MMEs vs. V9.02, Limb Effective PMD sensitivities vs. time (1 year average) Model: SCIATRAN (q,u)(R) m1 MPMD/MDET m2 m3 P. Liebing, IUP Bremen, SQWG PM4

PMD 7 Effective MMEs vs. V9.02, Limb Effective PMD sensitivities vs. time (1 year average) Model: SCIATRAN (q,u)(R) m1 MPMD/MDET m2 m3 P. Liebing, IUP Bremen, SQWG PM4

350/370 Effective MMEs vs. V9.02, Limb Effective 350/370 nm sensitivities vs. time (1 year average) Model: SCIATRAN (q,u)(R) m1 MPMD/MDET m2 m3 P. Liebing, IUP Bremen, SQWG PM4

V9.02 Degradation Correction SMR (State 62) Time Dependence of Irradiance after application of all corrections: Some wavelength vary by 1% or more! P. Liebing, IUP Bremen, SQWG PM4

SMR In-Band Signal SMR (State 62) SZA/AZ/Time/?? Dependence of PMD/Virtual Sum Ratio after application of all corrections P. Liebing, IUP Bremen, SQWG PM4

V8 Memory Effect? SMR (State 62) Time Dependence of Virtual Sum after application of all corrections: Offset for 1st readout in state: Memory effect? V8 L1b data! P. Liebing, IUP Bremen, SQWG PM4

Backup P. Liebing, IUP Bremen, SQWG PM4

Motivation For New Algorithm For channels 2,3,4 and 6 we only measure 1 Stokes component, but need 2 That 1 component is not in the direction we need (i.e., q) Need to make assumptions about the polarization angle Depending on assumptions and algorithm, large errors can be generated when the polarization angle is in the direction where “instrument” is not sensitive That happens more often than you think P. Liebing, IUP Bremen, SQWG PM4

Current Polarization Algorithm Original L0-1 algorithm: Problem when denominator small and/or u0/q0 large or q0 small P. Liebing, IUP Bremen, SQWG PM4

New Polarization Algorithm Change polarization frame so that u=0 (assumes known polarization angle) Rotate MM: Problem when denominator small (i.e., no polarization sensitivity in this direction) P. Liebing, IUP Bremen, SQWG PM4

Alternative for Limb and Insensitive Nadir Regions Assume a value for u, e.g., u=u(R) P fixed between 0.5 -1.5 or as f(R, TH, cosθ) Can in be applied in nadir for data with low sensitivity, too Use PARASOL slopes (?) Possibly slopes derived from yet another fit method of mine That would need yet another RTM reference for thick clouds P. Liebing, IUP Bremen, SQWG PM4