CONCLUSION - The impact of the fringe wash effects on the radiometric sensitivity as well as on the spatial resolution of the SMOS instrument has been.

Slides:



Advertisements
Similar presentations
Lim increasing HUT project Airborne f = 1.4 GHz = 21.3 cm U-shaped array rectangular freq. coverage cartesian grids 13 (vert.), 12 (hor.) 36 antennae Antenna.
Advertisements

Learning deformable models Yali Amit, University of Chicago Alain Trouvé, CMLA Cachan.
OSE meeting GODAE, Toulouse 4-5 June 2009 Interest of assimilating future Sea Surface Salinity measurements.
Antarctic Ice Shelf 3D Cross-sectional Imaging using MIMO Radar A. Hari Narayanan UCL Electronic and Electrical Engineering, UK P. Brennan UCL Electronic.
Resolution Resolving power Measuring of the ability of a sensor to distinguish between signals that are spatially near or spectrally similar.
ElectroScience Lab Studies of Radio Frequency Interference in SMOS Observations IGARSS 2011 Joel T. Johnson and Mustafa Aksoy Department of Electrical.
NASSP Masters 5003F - Computational Astronomy Lecture 13 Further with interferometry – Resolution and the field of view; Binning in frequency and.
Clouds and the Earth’s Radiant Energy System NASA Langley Research Center / Atmospheric Sciences Methodology to compare GERB- CERES filtered radiances.
Interferometric Spectral Line Imaging Martin Zwaan (Chapters of synthesis imaging book)
The Shapes Of Cross Correlation Interferometers Daniel Birman Boaz Chen
Imaging Algorithm – Eric Thiébaut – IAU Optical/IR Interferometry Working Group, 2002 J M M C Image Reconstruction in Optical/IR Aperture Synthesis Eric.
Volkan Cevher, Marco F. Duarte, and Richard G. Baraniuk European Signal Processing Conference 2008.
BMME 560 & BME 590I Medical Imaging: X-ray, CT, and Nuclear Methods Tomography Part 3.
Space Weather influence on satellite based navigation and precise positioning R. Warnant, S. Lejeune, M. Bavier Royal Observatory of Belgium Avenue Circulaire,
SELF CHARACTERIZATION OF MODELLING PARAMETERS FOR SYNTHETIC APERTURE IMAGING RADIOMETERS Eric ANTERRIEU, Serge GRATTON and Bruno PICARD CERFACS 42, avenue.
Texture Reading: Chapter 9 (skip 9.4) Key issue: How do we represent texture? Topics: –Texture segmentation –Texture-based matching –Texture synthesis.
CSE473/573 – Stereo Correspondence
Abstract In the case of the application of the Soil Moisture and Ocean Salinity (SMOS) mission to the field of hydrology, the question asked is the following:
Solar Polar Orbit Radio Telescope (SPORT): A Mission Concept for Interplanetary CMEs Imaging WU Ji, LIU Hao, SUN Weiying, ZHENG Jianhua, FENG Xueshang,
Universitat Politècnica de Catalunya INTERFEROMETRIC RADIOMETRY MEASUREMENT CONCEPT: THE VISIBILITY EQUATION I. Corbella, F. Torres, N. Duffo, M. Martín-Neira.
ElectroScience Lab IGARSS 2011 Vancouver Jul 26th, 2011 Chun-Sik Chae and Joel T. Johnson ElectroScience Laboratory Department of Electrical and Computer.
Phase Retrieval Applied to Asteroid Silhouette Characterization by Stellar Occultation Russell Trahan & David Hyland JPL Foundry Meeting – April 21, 2014.
© R.S. Lab, UPC IGARSS, Vancouver, July, 2011 OIL SLICKS DETECTION USING GNSS-R E. Valencia, A. Camps, H. Park, N. Rodríguez-Alvarez, X. Bosch-Lluis.
X. Bosch-Lluis 1, H. Park 2, A. Camps 2, S.C. Reising 1, S. Sahoo 1, S. Padmanabhan 3, N. Rodriguez-Alvarez 2, I. Ramos-Perez 2, and E. Valencia 2 1. Microwave.
Blue: Histogram of normalised deviation from “true” value; Red: Gaussian fit to histogram Presented at ESA Hyperspectral Workshop 2010, March 16-19, Frascati,
Ping Zhang, Zhen Li,Jianmin Zhou, Quan Chen, Bangsen Tian
Jul. 29, 2011IGARSS [3118] RELATION BETWEEN ROCK FAILURE MICROWAVE SIGNALS DETECTED BY AMSR-E AND A DISTRIBUTION OF RUPTURES GENERATED BY SEISMIC.
EXPERIMENTAL STUDY OF RADIO FREQUENCY INTERFERENCE DETECTION ALGORITHMS IN MICROWAVE RADIOMETRY José Miguel Tarongí Bauzá Giuseppe Forte Adriano Camps.
Telecom ParisTech Thursday, 28/07/11, Vancouver, Canada, IGARSS 2011 Extraction of water surfaces in simulated Ka-band SAR images of KaRIN on SWOT Fang.
Texture scale and image segmentation using wavelet filters Stability of the features Through the study of stability of the eigenvectors and the eigenvalues.
A. Montuori 1, M. Portabella 2, S. Guimbard 2, C. Gabarrò 2, M. Migliaccio 1 1 Dipartimento per le Tecnologie (DiT), University of Naples Parthenope, Italy.
A Frequency-Domain Approach to Registration Estimation in 3-D Space Phillip Curtis Pierre Payeur Vision, Imaging, Video and Autonomous Systems Research.
Fourier Depth of Field Cyril Soler, Kartic Subr, Frédo Durand, Nicolas Holzschuch, François Sillion INRIA, UC Irvine, MIT CSAIL.
Practical Poissonian-Gaussian Noise Modeling and Fitting for Single-image Raw-data Alessandro Foi, Mejdi Trimeche, Vladimir Katkovnik, and Karen Egiazarian.
Intrinsic Short Term Variability in W3-OH and W49N Hydroxyl Masers W.M. Goss National Radio Astronomy Observatory Socorro, New Mexico, USA A.A. Deshpande,
2011 IEEE International Geoscience And Remote Sensing Symposium IGARSS’11  July 24-29, 2011  Vancouver, C ANADA A synergy between SMOS & AQUARIUS: resampling.
SITE PARAMETERS RELEVANT FOR HIGH RESOLUTION IMAGING Marc Sarazin European Southern Observatory.
Study of Broadband Postbeamformer Interference Canceler Antenna Array Processor using Orthogonal Interference Beamformer Lal C. Godara and Presila Israt.
Design Features of a Boresighted GPM Core Radiometer Christopher S. Ruf Dept. of Atmospheric, Oceanic & Space Sciences University of Michigan, Ann Arbor,
Digital Image Processing CSC331 Image restoration 1.
SWOT Hydrology Workshop Ka-band Radar Scattering From Water and Layover Issues Delwyn Moller Ernesto Rodriguez Contributions from Daniel Esteban-Fernandez.
2D Sampling Goal: Represent a 2D function by a finite set of points.
© UPC IGARSS 2011 Vancouver July / 13 First results of the PAU Synthetic Aperture Radiometer I. Ramos-Perez, G. Forte. X. Bosch-Lluis, E.
Joint OS & SWH meeting in support of Wide-Swath Altimetry Measurements Washington D.C. – October 30th, 2006 Baptiste MOURRE ICM – Barcelona (Spain) Pierre.
NASSP Masters 5003F - Computational Astronomy Lecture 16 Further with interferometry – Digital correlation Earth-rotation synthesis and non-planar.
The Self-Coherent Camera: a focal plane wavefront sensor for EPICS
Doc.: IEEE /1229r1 Submission November 2009 Alexander Maltsev, IntelSlide 1 Application of 60 GHz Channel Models for Comparison of TGad Proposals.
Airborne gravimetry: An Introduction Madjid ABBASI Surveying Engineering Department, Zanjan University, Zanjan, Iran National Cartographic Center (NCC)
Digital Image Processing CSC331 Image restoration 1.
CS654: Digital Image Analysis Lecture 22: Image Restoration.
Optimal Relay Placement for Indoor Sensor Networks Cuiyao Xue †, Yanmin Zhu †, Lei Ni †, Minglu Li †, Bo Li ‡ † Shanghai Jiao Tong University ‡ HK University.
Universitat Politècnica de Catalunya CORRECTION OF SPATIAL ERRORS IN SMOS BRIGHTNESS TEMPERATURE IMAGES L. Wu, I. Corbella, F. Torres, N. Duffo, M. Martín-Neira.
M.P. Rupen, Synthesis Imaging Summer School, 18 June Cross Correlators Michael P. Rupen NRAO/Socorro.
M. Iorio 1, F. Fois 2, R. Mecozzi 1; R. Seu 1, E. Flamini 3 1 INFOCOM Dept., Università “La Sapienza”, Rome, Italy, 2 Thales Alenia Space Italy, Rome,
RECONSTRUCTION OF MULTI- SPECTRAL IMAGES USING MAP Gaurav.
Numericals.
Yun, Hyuk Jin. Theory A.Nonuniformity Model where at location x, v is the measured signal, u is the true signal emitted by the tissue, is an unknown.
NIRSpec Time Series Observations
Radio Coverage Prediction in Picocell Indoor Networks
Degradation/Restoration Model
Impact of reciprocal mixing on WUR performance
Telescopes and Images.
GOES-16 ABI Lunar Data Preparation to GIRO
San Diego Conference 2 August 2001
MODIS Characterization and Support Team Presented By Truman Wilson
Michael J. Jun Li#, Daniel K. Zhou%, and Timothy J.
Lecture 14 Figures from Gonzalez and Woods, Digital Image Processing, Second Edition, 2002.
Early calibration results of FY-4A/GIIRS during in-orbit testing
Goals of telescope: Radio `source’
IPSN19 杨景
Presentation transcript:

CONCLUSION - The impact of the fringe wash effects on the radiometric sensitivity as well as on the spatial resolution of the SMOS instrument has been estimated using two regularized reconstruction methods. These two approaches lead to similar results: provided the modelling of the fringe washing function is well-known and the reconstruction method is regularized, the influence of the spatial decorrelation effects are mitigated and the propagation of input noise is still under control. This remains true even with the digital correction proposed by Fishman et al. Finally, a hardware modification of the SMOS instrument is not necessary with regards to the fringe wash effects. REFERENCES M. A. F ISHMAN et al., “ How digital correlation affects the fringe washing function in L-band aperture synthesis radiometry’’, IEEE TGRS, 40(3), pp , E. A NTERRIEU, “Stabilized image reconstruction algorithm for synthetic aperture imaging radiometers”, Proc. IGARSS’02, Toronto (Canada), pp , ABSTRACT - It is now well established that Synthetic Aperture Imaging Radiometers (SAIR) promise to be powerful sensors for high-resolution observations of the Earth at low microwave frequencies. Within this context, the European Space Agency (ESA) is currently developing the SMOS space mission. A recent study has simulated fringe washing effects on a particular SAIR configuration, including the impact of coarse correlation. The results obtained with a simple inverse Fourier transform reconstruction have shown a large degradation of the spatial resolution as well as of the signal to noise ratio (SNR). In order to reduce the fringe washing effects, the authors have suggested to split the received signals into sub- signals with narrower bandwidths. In the particular frame of the SMOS space mission, the geometry and the dimensions of the instrument lead to a weaker influence of the fringe wash phenomenon on the image reconstruction. Furthermore, regularized reconstruction methods involving the modelling G-matrix allow to improve the quality of the reconstruction even when the signal is blurred by a radiometric noise. It is concluded that a hardware modification of the SMOS instrument is not necessary with regards to the fringe wash effects. ACKNOWLEDGMENTS This work is supported by ESA, CNES, CNRS and the Région Midi-Pyrénées. IMPACT OF THE FRINGE WASHING FUNCTION ON THE SPATIAL RESOLUTION AND ON THE RADIOMETRIC SENSITIVITY OF THE SMOS INSTRUMENT Bruno PICARD (1), Eric ANTERRIEU (1), Gérard CAUDAL (2) and Philippe WALDTEUFEL (3) (1) CERFACS 42 avenue Gaspard Coriolis Toulouse – FRANCE (3) IPSL-SA B.P Verrières le Buisson – France (2) IPSL-CETP avenue de l’Europe Vélizy – France distance from the center of the FOV [km] normalized brightness temperature distance from the center of the FOV [km] spatial resolution [km] instantaneous field of view (FOV) distance from the center of the FOV [km] normalized brightness temperature IMPACT OF THE FRINGE WASHING FUNCTION Simulations The mean values computed here for a realistic instrument with the regularized reconstruction methods are identical to those obtained for an ideal instrument with a simple Fourier transform. The fringe washing function does not degrade the performances of the instrument if the appropriate modelling is used, even in the case of the digital correction. Results for the baseline leading to the worth decorrelation effects for SMOS time lag t [ns] INSTRUMENT MODELLINGREGULARIZED RECONSTRUCTIONS physical regularization band-limited solution: mathematical regularization minimum norm solution: is the modelling operator is the experimental frequency coverage is the F OURIER transform operator is the projector onto the space of -band limited functions is the zero-padding operator beyond is the apodization window digital correlatorsanalog correlators The fringe washing function - accounts for spatial decorrelation effects - degrades SNR by reducing the amplitude of - maximum degradation for: - large spacing antennae (small details in FOV) - scene areas away from the center of the FOV is an ILL-POSED problem should be REGULARIZED to provide a UNIQUE and STABLE solution SAIR are band-limited imaging devices the objective is to restore: