SMOS: Principles of Operation of the MIRAS instrument Prof. A. Camps Dept. de Teoria del Senyal i Comunicacions Universitat Politècnica de Catalunya and IEEC/CRAE-UPC E-mail: camps@tsc.upc.edu …on behalf of many people (many anonymous) that kept this dream alive and make it happen devoted to Prof. Cal Swift… the pioneer SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 1/47 Outline of the presentation: 1. 2. Basic principles Imaging in Synthetic Aperture Radiometers: 2.1. Synthetic Aperture Radiometers 2.2. Image Reconstruction Algorithms: Ideal Case 3. 4. The SMOS Mission MIRAS instrument description 4.1. Array topology 4.2. Receivers’ architecture 4.3. NIR architecture 4.4. DIgital COrrelator System (DICOS) 4.5. CAlibration System (CAS) 5. Instrument Performance 5.1. Angular Resolution 5.2. Radiometric Performance: definition of terms 5.3. Image Formation Through a Fourier Synthesis Process 5.4. Imaging Modes: Dual-polarization and full-polarimetric 6. Geolocalization: from director cosines grid to Earth reference frame grid and Retrieval of Geophysical Parameters SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 2/47 1. Basic Principles • Spatial resolution is achieved by cross-correlating the signals collected by a number of antennas • Antennas can have a wide beam or a narrow one in one or two directions Channel 1 H1(f) b1(t) 1 b1b2* 2 H2(f) Channel 2 Baseline Complex Correlator V u,v = T ( , ) b2(t) 1 kB B1B2 G1G2 1 * b 1 t b2 t 2 Fn 1 , F *n 2 , TB , Tph rec 1 2 1 2 2 , sin cos, sin sin (u ,v ) (x , y ) 0 = antenna spacing normalized to the wavelength Ideal case: - Identical antenna patterns - Negligible spatial decorrelation - No antenna positioning errors SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 2D Fourier Transform V (u,v ) F T (, ) 3/47 2. Imaging in Synthetic Aperture Radiometers 2.1. Synthetic Aperture Radiometers using Fourier Synthesis: Radioastronomy VLA, New Mexico, Socorro Earth Observation (concept proposed in 1983 by LeVine & Good) ESTAR (1 D Aperture Synthesis) NASA MIRAS (2 D Aperture Synthesis) ESA V (u,v ) F T (, ) SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 4/47 • Differences between radio-astronomy and Earth observation: - Large antenna spacing - Very narrow field of view (FOV) - Obliquity factor (1/cos ) can be approximated by 1 - Antenna patterns are approximatedly constant (amplitude and phase) over the FOV - Typically quasi-point sources imaged over cold background super-resolution image reconstruction algorithms can be used SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 5/47 . After the successful results of ESTAR radiometer (1988), SSS image derived from the ’“Electronically Steered Thinned Array Radiometer (ESTAR)”. Error = 0.3 psu (D. M. LeVine et al., NASA Goddard). the European Space Agency starts in 1993 the first feasibility studies to apply synthetic aperture microwave radiometry in two dimensions: . MIRAS concept is born: Microwave Imaging Radiometer by Aperture Synthesis . First studies (1993-95): led by Matra Marconi Space as the prime contractor . 1995 Soil Moisture and Ocean Salinity Workshop (ESTEC, the Netherlands) Aperture Synthesis Microwave Radiometry is the only technique capable of measuring soil moisture and ocean salinity with enough accuracy and spatial resolution. SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 6/47 2.2. Image Reconstruction Algorithms: Ideal Case Antenna Positions Spatial frequencies (u,v) Periodic extension u v V (u,v ) F T (, ) Fn , TB , Tph rec 2 T ( , ) Overlapping of 1 alias Overlapping of 2 aliases Alias-free Field Of View (AF-FOV) 1 2 2 21 elements + 2 redundant elements/arm Antenna spacing d = 0.875 Hexagonal grid in (u,v) plane Nyquist criterion: d< / 3 SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 7/47 In SMOS the “alias-free FOV” can be enlarged since part of the alias images are the “cold” sky (including the galaxy!) TB image limited by Earth replicas Iso-incidence angle contours hsat=755.6 Km, =32.00º, d= 0.89 hsat=755.9 Km, tilt=32.50, d= 0.88 2 2.80 101.26 1200 1.5 2.26 81.39 1000 1 1.84 65.47 800 Along track coordinate(Km) 0.5 0 -0.5 -1 1.50 53.04 600 400 1.39 51.36 1.25 44.31 -1.5 2.47 88.01 2.21 78.62 2.31 81.55 2.13 74.95 1.76 61.13 1.72 50 58.77 1.40 40 46.29 1.43 48.48 1.19 30 37.53 1.20 39.69 20 1.34 48.11 1.39 48.00 200 -2 1 -3 -2 -1 0 1 2 3 0 0.8 0.4 Boresight Distance: 912.65 Km 0.2 Boresight Incidence Angle: 36.35º 0 0.1 0.2 Extension of Alias-Free FOV 0.3 0.4 1.13 40.12 1.27 40.33 1.10 32.62 10 1.05 34.97 1.20 32.85 1.23 35.52 1.39 35.77 0.6 0 60 0.5 0.6 1.49 39.34 -200 -800 0.7 0.8 0.9 -600 -400 -200 0 200 Cross track coordinate (Km) 400 600 800 1 - Pixel axial ratio a/b - Spatial resolution defined as geometric mean of axes 5.12 90.57 SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 8/47 3. The SMOS Mission SMOS is a challenge: Particularities of 2D aperture synthesis radiometers: 1) New type of instrument: - Review of the fundamental equation - Detail error model & error correction (calibration) algorithms - Image reconstruction algorithms 2) New type of observations: - Multi-look and multi-angle observations: . different pixel size and orientation . different noise and precision for each pixel - Polarization mixing: . Earth reference frame antenna reference frame 3) New L-band and multiangular ocean and soil emission models : - Wide range of incidence angles (0º-60º) 4) New geophysical parameter retrieval algorithms taking into account issues 1, 2 and 3 above SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 9/47 SMOS Mission: SMOS Scientific measurements require a - Sun-synchronous, - dawn/dusk, and - quasi circular orbit. Proba-2 Orbital parameters: • Mean altitude = 755.5 km • Eccentricity = 0.001165 • Mean inclination = 98.416º • Local Time Asc. Node =6 AM • Argument of Perigee = 90º • Mean Anomaly = 306.3º Transformed SS-19 missile Note: The SUN is nearly always visible (97 % of the time) !!! SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 10/47 4. MIRAS instrument description 4.1. Array topology Optical Splitter LCF_A_21 ARM A LCF_A_16 LCF_A_15 PD LCF_A_10 LCF_A_09 CMN • 69 antenna elements (LICEF) • Equally distributed over the 3 arms and hub • The acquired signal is transmitted to a central correlator unit, which computes the complex crosscorrelations of all signal pairs. Optical Splitter LCF_A_04 LICEF LCF_A_03 NS (DISTRIBUTED) LCF_AB_01 LCF_A_02 LCF_A_01 PD HUB In the arms In the Hub 3x3x6 3x4 66 - 3x1 3 CMN 3x3x1 3x1 12 CCU - 1 1 3x3x1 - 9 Unit LICEF ST CMN 1 SEGMENT OF ARM B PD Optical Splitter ST LICEF/NIR 1 SEGMENT OF ARM A LICEF/NIR NS (distributed) CMN LICEF/NIR NS (centralised) HUB NS (CENTRALISED) ARM B ARM C Optical Splitter CMN ST 1 SEGMENT OF ARM C LICEF Total NIR_AB_02 - 1 1 PD (2 to 8) 3x3x1 3x1 12 Optical Splitter (1 to 8) 3x3x1 3x1 12 Optical Splitter (2 to 12) - 1 1 TRANSMITTERS - 2 2 FILTERS - 2 2 X-ANTENNA - 1 1 LICEF/NIR SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 11/47 MIRAS consists of a central structure (hub) with 15 elements, and 3 deployable arms, each one having 3 segments with 6 antennas each. SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 [credits EADS-CASA] 12/47 CAL A e j UNCAL Offset 4.2. Receivers’ architecture: SLOPE IF ATTEN CORR. FILTER 1404-1423 MHz ANTENNA SWITCH ISOL LNA BPF RFAMP 1BIT ADC IF AMPs I DI MIXER TI H V C U DICOS 8-27 MHz TQ TRF Q DQ SYNTH MAIN PATH GAIN = 100 dB PMS PATH GAIN = 65 dB REF 55.84 MHz 1396 MHz DICOS VCO SLOPE IF ATTEN CORR. FILTER 1BIT ADC IF AMPs PMS • PMS acts as a total Power Radiometer in each LICEF TA aVout b • Needed to denormalize the “normalized” correlations (1 bit/2 level) SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 13/47 LICEF: the LIght and Cost Effective Front-end [credits MIER Comunicaciones] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 14/47 4.3. NIR architecture The Noise Injection Radiometer (NIR) is fully polarimetric and operates at 1.4 GHz 3 NIRs in the hub for redundancy. Functions: • precise measurement of Vpq(0,0) = TApq for mean value of TBpq(,) image. • measurement of noise temperature level of the reference noise source of Calibration Subsystem (CAS) absolute amplitude reference 1st LICEF unit (V-pol) Correlated noise inputs (from Noise Distribution Network) allow phase/amplitude calibration of receivers as LICEFs & for 3rd and 4th Stokes parameters measurements Controller unit (switches, noise injection...) 2nd LICEF unit (H-pol) [credits TKK] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 15/47 SMOS NIR: [Colliander et al., 2005] Normal mode of operation: Calibrating internal noise source mode: known (cold sky) T NA + TA = TU SMOS: Principles of Operation & First Results ? T NA + TA = TREF + TNR ICMARS 2010 Jodhpur – India December 16th, 2010 [credits HUT] 16/47 4.4. DIgital COrrelator System (DICOS) 1 bit ADC (comparator) in each LICEF Correlator = = NOT-XOR + up-counter Digital signals from each LICEF are transmitted to DICOS to compute the complex cross-correlations of all signal pairs. SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 17/47 • Lower half: II-correlations: Nr,Nc Zr r Vr • Upper half: IQ-correlations: Ni,Nc Zi i Vi • Diagonal: IQ-correlations of same element (q: quadrature errors) • Correlations of I and Q signals with 0’s and 1’s to compensate comparators’ threshold errors • Correlations of 0’s and 0’s and 1’s and 1’s = Ncmax • NCmax = 65437 for dual-pol mode (= fCLK · int) NCmax = 43625 for full-pol mode •Total number of products: •2556 correlations Ik-Ij •2556 correlations Ik-Qj •72 correlations Ik-Qk •72 correlations I-0 •72 correlations Q-0 •72 correlations I-1 •48 correlations Q-1 •36 control correlations between 1 and 0 channels (4 for each ASIC) SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 18/47 CCU: the Correlator and Control Unit [credits EADS-CASA] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 19/47 4.5. CAlibration System (CAS) Noise sources needed to calibrate the instrument. HUB SMOS: Principles of Operation & First Results ARMS ICMARS 2010 Jodhpur – India December 16th, 2010 20/47 Centralized and distributed calibration Correlated noise is injected to the receivers in two steps: first the “even” sources and then using the “odd” ones 48 Overlapping between elements (phase & amplitude tracking along the arms) * source 0 * source 2 * source 5 * source 8 B Centralized Calibration (separable & non-separable errors can be corrected) Distributed Calibration (only separable errors can be corrected) 49 A 24 1 25 C These receivers belong to the NIR (□: H-channel) and do not form additional baselines Overlapping between elements (phase & amplitude tracking among arms) 72 SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 21/47 OVERALL SEGMENT ARCHITECTURE SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 [credits EADS-CASA] 22/47 6 LICEF / segment SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 [credits EADS-CASA] 23/47 MOHA SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 [credits EADS-CASA] 24/47 CAS SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 [credits EADS-CASA] 25/47 CMN SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 [credits EADS-CASA] 26/47 5. Instrument Performance 5.1. Angular Resolution V (u, v ) = 1 12 T , T B ph rec F n1 ( , )Fn*2 ( , ) 1 2 2 2 2 1 u v -j 2 u +v d d r n12 e f0 • The “ideal” brightness temperature image is formed by an inverse (discrete) Fourier transform of the measured visibility samples (B = 0): 1 j 2 u v Tˆ , s W umn , v mn V 0 umn ,v mn e mn mn T ' , ' K m n ' 2 ' 2 1 AF 0 ', ' d ' d ' Equivalent Array Factor: same response as for an array of elements at (u,v) positions (except for the |(.)|2) j 2 umn ' v mn ' 3 2 s d 2 AF 0 ', ' s W umn , v mn e m n • The retrieved Τ̂ , image is the 2D convolution of the original T(,) image with the instrument’s impulse response or equivalent array factor: Τ̂ , = FH1 W u,v V 0 u, v = AF 0 , * Τ , SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 27/47 Response with rectangular window rect 3 dB 2 umax ; e 10% for umax 15 umax 2 3NEL d MBE 43% Response with Blackmann window (rotational symmetry) Blackmann 1.48 rect 3 dB 3 dB MBE 90% TA' MBE Tmain lobe 1 MBE Tsec ondary lobes SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 W(umn,vmn): window to weight the visibility samples: • reduces side lobes • widens main lobe • increases main beam efficiency (MBE) 28/47 5.2. Radiometric Performance: definition of terms Error maps: TB(,,t) Random errors (noise due to finite integration time) Systematic errors (instrumental errors) Temporal average Zero Temporal standard deviation Radiometric sensitivity Spatial average Radiometric bias (scene bias) Spatial standard deviation Radiometric accuracy (pixel bias) SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 0 M Tsensitivit y Tbias T̂ , , t T̂ , , t B i B t i1 M 1 2 1 N T̂B i , i , t TB i , i N i1 t N Taccuracy i 1 T̂B i , i , t 2 t TB i , i N 1 29/47 Radiometric Sensitivity over ocean Dashed lines. Theoretical formula: TB ( , ) 3 2 TA TR a d 1 2 2 w N 2 B eff t ( , ) Cut for =0 [credits I. Corbella] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 30/47 Galaxy Alias Moon Cosmic Background Radiation at 3.3 K Scene Bias < 0.1 K Accuracy < 0.5 K Sun Alias Galaxy (yellowish) Galactic radiosource (TBC) [credits DEIMOS] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 31/47 Incidence angle dependence Singularity in the transformation antenna to Earth reference frame (dual-pol mode) • 45 deg singularity discarded • All points with the same incidence angle averaged TX cos 2 sin 2 TH T 2 2 Y sin cos TV Fresnel [credits I. Corbella] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 32/47 5.3. Image Formation Through a Fourier Synthesis Process Even in the ideal case: - Antenna spacing > /3 aliasing - Gibbs phenomenon near the sharp transitions (mainly alias borders) In the real case: - Antenna patterns are different - Receivers’ frequency responses are different ( FWF different) - Antenna positioning errors (u,v,w)real different from (u,v,0)ideal IHFFT cannot be used as image reconstruction method More sophisticated algorithms must be devised But it will be good that the second ones tend to IHFFT in ideal conditions … and obviously instrumental errors must be calibrated first! SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 33/47 Real Aperture Radiometer: 1 step calibration TB imaging pixel by pixel through antenna scan: 1) Aperture Synthesis Radiometer: 2 step calibration TB imaging in a single snap-shot (1 integration time = 1.2 s / polarization in dual-pol): 1) Receivers relative calibration (image “contrast”) - Error model (distorsions, artifacts, blurring…) - Internal references (Tcorr, Tuncorr,…) Absolute calibration External references: Thot, Tcold *** Imaging by (e.g.) conical scan *** *** Image Reconstruction Algorithm *** 2) Absolute Calibration (image accuracy) - External references (FTT, OTT…) - Thot/Tcold, ground truth, external calibration… SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 34/47 Calibration Concept: Brief sketch • • Items that need calibration: - NIR Gain and Offset - PMS gain and offset (receiver and baseline amplitude errors) - Fringe-washing function FWF (amplitude and phase errors) - Noise that is injected to receivers during calibration - Correlator Offsets Types of Calibration: – Internal: injection of correlated or uncorrelated noise to the receivers – External: observation of known target: • NIR absolute calibration • Flat-Target Transformation: to calibrate antenna pattern errors – CAS Calibration: performed by NIR during internal calibration – Correlator Calibration: injecting known signals SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 35/47 a. MIRAS internal calibration Instrumental errors correction: set of measurements and mathematical relations to remove instrumental errors INTERNAL INSTRUMENT CALIBRATION Error model • Characterizes the instrument behavior independently of the input signal. • It can be characterized by suitable internal known signals injected at its input: correlated/uncorrelated and hot/cold noise injection. SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 36/47 MIRAS Internal calibration PMS gain PMS offset LICEF PMS Matched load Hot Mixer i ADC IF-i H CC vk GkTsys voffk k To correlator matrix Antenna switch U v L RF V C q ADC IF-q TS1 TS2 Noise distribution network 0 N LO distribution C Reference receiver (Noise Injection Radiometer) H Noise source V NIR Warm (*) Clock distribution Tˆkj Sk 0 S *j 0TS Sk 0 S *j 0Tn CC sysk T T T C Nk C Rk 2 TN k S k 0 TS Tn (1 S k 0 ) 2 SMOS: Principles of Operation & First Results (*) Tˆkj Gkj M C kj Correlation amplitude CC CC Tsys T k sys j Calibrated visibility: TN Vˆkj AC sysk T ICMARS 2010 Jodhpur – India December 16th, 2010 1 * SCAk SCA j M kjA TsysACk TsysACj Gkj vk voffk Gk 37/47 Formulation of the Problem: Instrument Equation After Internal Calibration pq 12 V 1 12 1 2 2 Tpq , Trec pq 1 2 2 Fnp1 , F * np 2 fore exp j 2 u12 v12 w12 1 2 2 2 u v w 2 12 12 12 1 , r12 f0 d d Phase of fringe-washing function Amplitude of fringe-washing functions 8 1.05 To be corrected using the Flat Target Response 1 4 0.9 pp ij 2 0.85 Deg pp ij 6 0.95 V (u,v ) V (u,v ) V (u,v ) pp ij 0 0.8 0.75 W u, v V u,v G T dec , -2 0.7 -4 0.65 0.6 -30 -20 -10 0 time (ns) 10 20 30 -6 -30 -20 -10 0 time (ns) 10 20 [credits I. Corbella] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 38/47 30 The Flat Target Response: -The Flat Target Response is defined by: Vij ,pq (u,v;1) 1 i j Fn,i,p ( , )Fn, j,q * ( , ) 2 1 2 u v j 2 (u v ) rij d d e 2 2 fo 1 1 Vijpq (u,v;To Tr ) To Tr Vij ,pq (u,v; 1) defining: TBpp Tr pp V (u,v ) Vij (u,v ; TP Tr) TP Tr pp ij Then the differential visibilities to be processed are: Vijpp (u,v ) Vijpp (u,v ) Vijpp (u,v ) SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 39/47 External calibration • Once in a month (every week during commissioning) the platform rotates to point to the cold sky • External calibration is used to correct for elements not included in internal calibration: switch and antenna losses • Also the Noise Injection Radiometer (NIR) is calibrated and the Flat Target Response (FTR) measured HERE IT GOES THE ANIMATION. T_X_skylook2.gif HERE IT GOES THE ANIMATION. T_Y_skylook2.gif Tx and Ty while satellite is turning up SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 [credits I. Corbella] 40/47 5.4. Imaging Modes: Dual-polarization and full-polarimetric Dual-polarization radiometer: MIRAS has dual-pol antennas, but only one receiver polarizations have to be measured sequentially, with an integration time of 1.2 s each [credits M. Martin-Neira] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 41/47 Full-polarimetric mode: (selected as operational mode for SMOS) [credits M. Martin-Neira] SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 42/47 6. Geolocalization and Retrieval of Geophysical Parameters 6. Geolocalization: from director cosines grid to Earth reference frame grid • ISEA family of grids seem to be the best option for the SMOS Products, but EASE-Grid has come to be popular amongst many of the Earth Observation missions of the USA, namely AQUA (NASA/NASDA) and AQUARIUS (NASA), which are particularly interesting for comparison with the SMOS products. • Spatial partitioning of EASE-Grid is square-based and ISEA can be triangular, hexagonal or diamond-based: - In its hexagonal form, ISEA has a higher degree of compactness, quantize the plane with the smallest average error and provides the greatest angular resolution. -ISEA hexagonal possesses uniform adjacency with its neighbors, unlike the square EASE-Grid. • Both grids have uniform alignment and are based on a spherical Earth assumption. • ISEA hexagonal at aperture 4 and resolution 9 (15km) is made up of 2,621,442 points and the EASE-Grid at 12km has 3,244,518 points. • EASE-Grid is congruent, whereas ISEA is not congruent, being impossible to decompose a hexagon into smaller hexagons or aggregate hexagons into larger ones. This would be a negative feature for real-time re-gridding, but in SMOS the grids will be pre-generated. SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 43/47 Auxiliary data Snap-shot 1 OS map (1 overpass) Spatio-temporal averaging Snap-shot 2 Snap-shot 3 Multi-angular emission models SM map (1 overpass) Snap-shot 4 L1 processor L2 processor L3 processor • Atmospheric and foreign sources corrections • Use of multiangular information: 1. Th & Tv or Tx and Ty + Faraday and geometric rotations corrections: Earth Antenna: retrieval in antenna ref frame, Antenna Earth: retrieval in Earth ref frame, 2. First Stokes parameter: I = Tx+Ty=Th+Tv. (invariant to rotations) SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 44/47 • Sample SMOS data: Pixel in different positions of SMOS swath (pin 3) (pin 5) SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 OS retrieval: 45/47 • Sample SMOS data over Australia: Murrumbidge catchement 40 km SMOS soil moisture [m3/m3] 60 km 1 km downscaled SMOS soil moisture [m3/m3] using MODIS VIS/IR data (a) Murrumbidgee catchment (b) MODIS NDVI [m3/m3] (c) MODIS LST [m3/m3] (a) 60 x 60 km Yanco site in the Murrumbidgee catchment, SouthEastern Australia, (b) 1 km MODIS NDVI, and (c) and LST [K] on January 19, 2010. SMOS: Principles of Operation & First Results Sample results of the application of the downscaling algorithm to a SMOS image covering the Murrumbidgee catchment, South-Eastern Australia, on January 19, 2010 (6 am). First row: 40 km SMOS soil moisture [m3/m3] over Murrumbidgee (left), and zoom into Yanco site (right). Second row: 1 km downscaled soil moisture [m3/m3] over Murrumbidgee (left), and zoom into Yanco site (right). Dots indicate the location of the soil moisture permanent stations within the Murrumbidgee catchment used for validation purposes with colors representing their measurement at the exact SMOS acquisition time (only within Yanco site). Empty areas in the images correspond to non-retrieved soil moisture or clouds masking MODIS Ts measurements. ICMARS 2010 Jodhpur – India December 16th, 2010 46/47 Thanks for your attention! SMOS: Principles of Operation & First Results ICMARS 2010 Jodhpur – India December 16th, 2010 47/47