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General methodology for the derivation of high resolution oceanic data through information fusion at different scales

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General methodology for the derivation of high resolution oceanic data through information fusion at

different scales

Hussein Yahia, Joel Sudre, Ismael Hernandez-Carrasco, Dharmendra Singh, Nicolas Brodu, Christoph Garbe, Veronique Garçon

To cite this version:

Hussein Yahia, Joel Sudre, Ismael Hernandez-Carrasco, Dharmendra Singh, Nicolas Brodu, et al..

General methodology for the derivation of high resolution oceanic data through information fusion

at different scales. ESA Living Planet Symposium 2016, May 2016, Prague, Czech Republic. �hal-

01217596�

(2)

References

- [1] H. Yahia, J. Sudre, C. Pottier and V. Garçon, 2010, Motion analysis in oceanographic satellite images using multiscale methods and the energy cascade, Pattern Recognition, DOI: 10.1016/J.patcog.2010.04.011

- [2] J. Sudre, H. Yahia, O. Pont, and V. Garçon, 2015, Ocean turbulent dynamics at superresolution from optimal multiresolution analysis and multiplicative cascade, IEEE TGRS, DOI: 10.1109/TGRS.2015.2436431

- [3] I. Hernández-Carrasco, J. Sudre, V. Garçon, H. Yahia, C. Garbe, A. Paulmier, B. Dewitte, S. Illig, I. Dadou, M. González-Dávila, and J.

M. Santana-Casiano, 2015, Reconstruction of super-resolution ocean pCO2 and air-sea fluxes of CO2 from satellite imagery in the southeastern Atlantic, Biogeosciences, DOI: 10.5194/bg-12-5229-2015

Funding

This work is supported by ESA and CNES funding through the ESA Support To Science Element Grant 4000014715/11/I-NB Oceanflux- Upwelling and the OST-ST/ TOSCA ICARODE proposal.

Abstract

Derivation of high-resolution (HR) spatial distribution of data is a fundamental problem in Earth Observation. The problem can be solved through information fusion at different scales.

New method based on an approximation of the energy of Microcanonical Cascade (MC), expressed in a Multiscale Microcanonical Formulation (MMF), for physical intensive variables of Fully Developed Turbulence (FDT) encountered in satellite Oceanography and Ocean/Climate interactions.

The generality of the approach offers the opportunity to infer different oceanic turbulent signals from Low Resolution (LR) to HR. Basic idea:

- optimal cascading to decrease the spatial resolution of the HR signal,

- use the signal available at LR, transmit that information along the scales back to higher spatial resolution using the cascade to obtain a new HR signal.

The process has been successfully used to obtain oceanic currents [1,2], oceanic partial pressure of CO

2

[3].

Extension to many Essential Climate Variables both in the ocean and atmosphere critical for characterizing Earth’s climate and its changes.

Conclusion and Future Work

Evidencing multiscale geometric structures in synthetic ROMS data and satellite data data through the Multiscale Microcanonical Formalism

Validation of algorithms on synthetic ROMS data Application of the algorithms on satellite data Validation of the new HR satellite data with in-situ data

Future Work: Application of this general method for Altimetry (SWOT project submitted on OST- ST/TOSCA)

Area of Synthetic ROMS data

HR Signal with FDT

Replace the approximation of the signal by LR Information to make the inference

Microcanonical Cascade with its Optimal Wavelet Microcanonical Cascade

with its Optimal Wavelet

New HR inferred signal

Keep horizontal vertical &

diagonal coefficients Keep horizontal vertical &

diagonal coefficients

o

Obtain a relevant signal with SST and MMF to carry through the resolution (descent)

o

Carry back through the resolution (ascent) a new signal only known at LR General concept of the MMF/MC method

General methodology for the derivation of high resolution oceanic data through information fusion at different scales

OCEA-76

H. Yahia 2 , J. Sudre 1 , I. Hernandez-Carrasco 1,3 , D. Singh 2,4 , N. Brodu 2 , C. Garbe 5 , V. Garçon 1

1

LEGOS/CNRS, France,

2

INRIA Centre-Bordeaux Sud-Ouest, France,

3

IMEDEA, Spain,

4

Indian Institute of Technology, India,

5

IWR/University of Heidelberg, Germany

Relationship between the different oceanic signals:

To use the general concept ( ), we need to verify the « linearity » between HR and LR signals.

Examples of synthetic data from ROMS

SE SST

SE SST

SE pCO2

SST Chl-a

pCO2 pCO2

The properties diagrams using 10 years of ROMS data : Complex relationship between

the different data.

Cannot use directly the data to apply the method described in

( )

Compute the Singularity Exponents (SE) of each signal by using a functional.

SE corresponds to h(x) in the functional:

SE pCO2

SE Chl-a SE pCO2

The properties diagrams using 10 years of singularity exponents of ROMS data : series of linear relationship Use the SE of oceanographic

data to apply the method described in ( )

Method to obtain HR pCO

2

using HR SST, HR Chl-a, LR pCO

2

1) A(x) SE_SSTHR(x,t) + B(x) SE_ChlHR(x,t) + C(x) SE_pCO2LR(x,t) + D(x) = Proxy[SE_pCO2HR(x,t)]

A(x),B(x),C(x), D(x): coefficients of the multi-linear regression computed using Roms data 2) Apply the general concept to the Proxy[SE_pCO2HR(x,t)] :

For each time t, compute SE of satellite data,

Injection in the multi-linear regression above to obtain the Proxy[SE_pCO2HR(x,t)]

Use the proxy as « HR signal with FDT », and the pCO2LR replace the approximation coefficients in the general concept.

This method is fully described and validated within-situ data in [3].

HR

U Exp

∇( )π/2

Exp )

HR/2

(

π

Microcanonical Cascade

LR

U Exp

∇( )π/2

UHR (Fluid Exponent)

SST HR

Microcanonical Cascade Singularity Exponent of

SSTHR

Microcanonical Cascade (Fluid Exponent)

SST HR

Stream Function [Isern-Fontanet et al. 2007]

Singularity Exponent of SSTHR

Microcanonical Cascade Stream FunctionHR

HR

U r

LR

U r

To obtain Oceanic current at HR : Separation of Norm and Direction (See [1,2] for full description and validation with in-situ data)

Direction Algorithm Norm Algorithm

Examples of data obtained by the MMF/MC method

Maps of : a) absolute dynamic topography at 1/4° and the LR current (geostrophic and Ekman components) associated b) inferred HR current at 1/24° [1,2]

c) LR ocean pCO2 from Carbon Tracker at 1°

d) inferred HR pCO2 at 1/32° [3]

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