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HAL Id: hal-00638825 https://hal.archives-ouvertes.fr/hal-00638825 Submitted on 7 Nov 2011 HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés. Optimal Parameter Estimation in Heterogeneous Clutter for High Resolution Polarimetric SAR Data Gabriel Vasile, Frédéric Pascal, Jean-Philippe Ovarlez, Pierre Formont, Michel Gay To cite this version: Gabriel Vasile, Frédéric Pascal, Jean-Philippe Ovarlez, Pierre Formont, Michel Gay. Optimal Pa- rameter Estimation in Heterogeneous Clutter for High Resolution Polarimetric SAR Data. IEEE Geoscience and Remote Sensing Letters, IEEE - Institute of Electrical and Electronics Engineers, 2011, 8 (6), pp.1046-1050. 10.1109/LGRS.2011.2152363. hal-00638825

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Page 1: Optimal Parameter Estimation in Heterogeneous Clutter for High … · 2021. 2. 18. · Clutter for High Resolution Polarimetric SAR Data Gabriel Vasile, Member, IEEE, Fre´de´ric

HAL Id: hal-00638825https://hal.archives-ouvertes.fr/hal-00638825

Submitted on 7 Nov 2011

HAL is a multi-disciplinary open accessarchive for the deposit and dissemination of sci-entific research documents, whether they are pub-lished or not. The documents may come fromteaching and research institutions in France orabroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, estdestinée au dépôt et à la diffusion de documentsscientifiques de niveau recherche, publiés ou non,émanant des établissements d’enseignement et derecherche français ou étrangers, des laboratoirespublics ou privés.

Optimal Parameter Estimation in HeterogeneousClutter for High Resolution Polarimetric SAR Data

Gabriel Vasile, Frédéric Pascal, Jean-Philippe Ovarlez, Pierre Formont, MichelGay

To cite this version:Gabriel Vasile, Frédéric Pascal, Jean-Philippe Ovarlez, Pierre Formont, Michel Gay. Optimal Pa-rameter Estimation in Heterogeneous Clutter for High Resolution Polarimetric SAR Data. IEEEGeoscience and Remote Sensing Letters, IEEE - Institute of Electrical and Electronics Engineers,2011, 8 (6), pp.1046-1050. �10.1109/LGRS.2011.2152363�. �hal-00638825�

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Optimal Parameter Estimation in HeterogeneousClutter for High Resolution Polarimetric SAR Data

Gabriel Vasile,Member, IEEE, Frederic Pascal,Member, IEEE, Jean-Philippe Ovarlez,Member, IEEE,Pierre Formont,Student Member, IEEE Michel Gay,Member, IEEE

Abstract—This paper presents a new estimation scheme for op-timally deriving clutter parameters with high resolution P OLSARdata. The heterogeneous clutter in POLSAR data is describedby the Spherically Invariant Random Vectors model. Threeparameters are introduced for the high resolution POLSARdata clutter: the span, the normalized texture and the specklenormalized covariance matrix. The asymptotic distribution of thenovel span estimator is investigated. A novel heterogeneity testfor the POLSAR clutter is also discussed. The proposed methodis tested with airborne POLSAR images provided by the ONERARAMSES system.

Index Terms—Estimation, detection, polarimetry, SAR.

I. I NTRODUCTION

The recently launched polarimetric SAR (POLSAR) sys-tems are now capable of producing high quality images ofthe Earth’s surface with meter resolution. The goal of theestimation process is to derive the scene signature from theobserved data set. In the case of spatially changing surfaces(”heterogeneous” or ”textured” scenes) the first step is to de-fine an appropriate model describing the dependency betweenthe polarimetric signature and the observable as a functionof the speckle. In general, the multiplicative model has beenemployed for POLSAR data processing as a product betweenthe square root of a scalar positive quantity (texture) and thedescription of an equivalent homogeneous surface (speckle)[1], [2].

In the context of the non-Gaussian polarimetric cluttermodels, several studies tackled POLSAR parameter estimationusing the product model. For deterministic texture, Novakand Burl derived the Polarimetric Whitening Filter (PWF)by optimally combining the elements of the polarimetriccovariance matrix to produce a single scalar image [1], [3].Using the complex Wishart distribution, the PWF for homo-geneous surfaces has been generalized to an Multi-look PWF(MPWF) in [2], [4]. The objective of this paper is to present anovel parameter estimation technique based on the Spherically

G. Vasile and M. Gay are with the Grenoble-Image-sPeech-Signal-Automatics Lab (GIPSA-lab), CNRS, Grenoble, France (e-mail:[email protected]; [email protected])

F. Pascal is with the Supelec, National University of Singapore, DefenceScience and Technology Agency Research Alliance, SONDRA, Gif-sur-Yvette, France (e-mail: [email protected])

J.-P. Ovarlez and P. Formont are with the French Aerospace Lab(ONERA), DEMR/TSI, Palaiseau, France and with the Supelec, NationalUniversity of Singapore, Defence Science and Technology Agency ResearchAlliance, SONDRA, Gif-sur-Yvette, France (e-mail: [email protected];[email protected])

Invariant Random Vectors (SIRV) model. For a detailed reviewon the use of SIRV with POLSAR data refer to [5].

This paper is organized as follows. The POLSAR param-eter estimation strategy for SIRV clutter model both withnormalized texture, and with normalized covariance matrixispresented in Sect. II and Sect. III, respectively. Then, thenovelspan estimator is introduced in Sect. IV. Next, some estimationresults are shown in Sect. V on a real high-resolution POLSARdataset acquired by the ONERA RAMSES system. Eventually,in Sect. VI, some conclusions are presented.

II. SIRV CLUTTER MODEL WITH NORMALIZED TEXTURE

The SIRV is a class of non-homogeneous Gaussian pro-cesses with random variance [6], [7]. The complexm-dimensional measurementk (m being the number of po-larimetric channels) is defined as the product between theindependent complex circular Gaussian vectorζ ∼ N (0, [T ])(speckle) with zero mean and covariance matrix[T ] = E{ζζ†}and the square root of the positive random variableξ (repre-senting the texture):k =

√ξ · ζ. It is important to notice that

in the SIRV definition, the probability density function (PDF)of the texture random variable is not explicitly specified. Asa consequence, SIRVs describe a whole class of stochasticprocesses [8].

For POLSAR clutter, the SIRV product model is the productof two separate random processes operating across two differ-ent statistical axes [5]. The polarimetric diversity is modeledby the multidimensional Gaussian kernel. The randomnessof spatial variations in the radar backscattering from celltocell is characterized byξ. Relatively to the polarimetric axis,the texture random variableξ can be viewed as a unknowndeterministic parameter from cell to cell.

The texture and the covariance matrix unknown param-eters can be estimated from the ML theory. ForN i.i.d.(independent and identically distributed) secondary data,let Lk(k1, ...,kN |[T ], ξ1, ..., ξN ) be the likelihood function tomaximize with respect to[T ] andξi.

Lk(k1, ...,kN ; [T ], ξ1, ..., ξN ) =1

πmN det{[T ]}N×

×N∏

i=1

1

ξmi

exp

(−k

†i [T ]−1

ki

ξi

). (1)

The corresponding ML estimators are given by [9]:

∂lnLk(k1, ..., kN |[T ], ξ1, ..., ξN)

∂ξi

= 0 ⇔ bξi =k†i [T ]−1

ki

m, (2)

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∂lnLk(k1, ..., kN |[T ], ξ1, ..., ξN)

∂[T ]= 0 ⇔ [ bT ] =

1

N

NX

i=1

kik†i

bξi

. (3)

As the variablesξi are unknown, the following normal-ization constraint on the texture parameters assures that theML estimator of the speckle covariance matrix is the SampleCovariance Matrix (SCM):

[ bT ] =1

N

NX

i=1

kik†i = [ bT ]SCM ⇔

1

N

NX

i=1

kik†i

1 −1

bξi

«

= [0m].

(4)The generalized ML estimator forξi are obtained by intro-

ducing Eq. 4 in Eq. 2:

ξi =k†i [T ]−1

SCMki

m. (5)

Note theki primary data is the cell under study.The normalized texture estimator from Eq. 5 is known as

the Polarimetric Whitening Filter (PWF-SCM) introduced byNovak and Burl in [1].

III. SIRV CLUTTER MODEL WITH NORMALIZED

COVARIANCE MATRIX

Let now the covariance matrix be of the form[T ] = σ0[M ],such that Tr{[M ]} = 1. The product model can be also writtenask =

√τ ·z, wherez ∼ N (0, [M ]). σ0 andξ are two scalar

positive random variables such thatτ = σ0 · ξ.Using the same procedure as in Sect. II and given the fact

that the covariance matrix is normalized, it is possible tocompute the generalized ML estimator of[M ] as the solutionof the following recursive equation:

[M ]FP = f([M ]FP ) =1

N

N∑

i=1

kik†i

k†i [M ]−1

FP ki

. (6)

This approach has been used in [10] by Conte et al. to derivea recursive algorithm for estimating the matrix[M ]. Thisalgorithm consists in computing the Fixed Point off usingthe sequence([M ]i)i≥0 defined by:

[M ]i+1 = f([M ]i). (7)

This study has been completed by the work of Pascal et al.[11], [12], which recently established the existence and theuniqueness, up to a scalar factor, of the Fixed Point estimatorof the normalized covariance matrix, as well as the conver-gence of the recursive algorithm whatever the initialization.The algorithm can therefore be initialized with the identitymatrix [M ]0 = [Im].

The generalized ML estimator (PWF-FP) for theτi texturefor the primary dataki is given by:

τi =k†i [M ]−1

FPki

m. (8)

One can observe that the PWF-FP texture from Eq. 8 hasthe same form as the PWF-SCM. The only difference is theuse of the normalized covariance estimate given by the FPestimator instead of the conventional SCM [5].

IV. M AIN RESULT

The span (total power)σ0 can be derived using the covari-ance matrix estimators presented in Sect. II and Sect. III as:

σ0 =k†[M ]−1

FPk

k†[T ]−1SCMk

. (9)

Note that Eq. 9 is valid when consideringN identicallydistributed linearly independent secondary data and one pri-mary data. It can be seen as a double polarimetric whiteningfilter issued from two equivalent SIRV clutter models: withnormalized texture variables and with normalized covariancematrix parameter.

The main advantage of the proposed estimation scheme isthat it can be directly applied with standard boxcar neighbor-hoods.

A. Asymptotic statistics of σ0

This section is dedicated to the study of large sampleproperties and approximations of the span estimatorσ0 formEq. 9.

On one hand, the asymptotic distribution of the FP estimatorfrom Eq. 6 has been derived in [12]. The FP estimatorcomputed withN secondary data converges in distribution tothe normalized SCM computed withN [m/(m+1)] secondarydata. Since the normalized SCM is the SCM up to a scalefactor, we may conclude that, in problems invariant withrespect to a scale factor on the covariance matrix, the FPestimate is asymptotically equivalent to the SCM computedwith N [m/(m + 1)] secondary data. Hence one can setthe degrees of freedom of FP normalized covariance matrixestimators as:

q1 = Nm

m + 1. (10)

On the other hand, Chatelain et al. establishedthe multi-sensor bivariate gamma distribution PDF, whose marginsare univariate gamma distributions with different shapeparameters [13]:

PbΓ(y1, y2; p1, p2, p12, q1, q2).

The scale parametersp2 and p1, the shape parametersq2 >q1 and p12 are linked to the mean parametersµ1, µ2, to thenumber of degrees of freedomn1, n2, and to the normalizedcorrelation coefficientρ such as:

q1 = n1, q2 = n2, p1 =µ1

q1, p2 =

µ2

q2, p12 =

µ1µ2

q1q2(1 − ρ).

Using these results, we derived the PDF of the ratioR =y1/y2 of two correlated Gamma random variables:

PRΓ(R, p1, p2, p12, q1, q2) = Rq1−1

(p2

p12

)q1(

1

p2

)q2

×

×(

p12

p1 + Rp2

)q2+q1 Γ(q1 + q2)

Γ(q1)Γ(q2)× (11)

× H3

[q1 + q2, q2 − q1, q2; R

p1p2 − p12

(p1 + Rp2)2,

p1p2 − p12

p2(p1 + Rp2)

],

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where H3(α, β, γ; x, y) =

∞∑

m,n=0

(α)2m+n(β)n

(γ)m+nm!n!xmyn is

one of the twenty convergent confluent hypergeometric seriesof order two (Horn function), and(α)n is the Pochhammersymbol such that(a)0 = 1 and(a)k+1 = (a + k)(a)k for anypositive integerk [14].

By taking into consideration both Eqs. 10, 11 and theCochran’s theorem [15], the PDF of the span estimatorfrom Eq. 9 converges asymptotically to the the ratio of twocorrelated Gamma random variables PDF (the ratio of twoquadratics). Moreover, the degrees of freedomn1 andn2 areset toN [m/(m + 1)] andN (the number of secondary data),respectively.

1 2 3 4 5 6 70

0.2

0.4

0.6

0.8

Empirical PDFP(σ

0; µ=3, N=24, m=3, ρ=0.05)

P(σ0; µ=3, N=24, m=3, ρ=0.5)

P(σ0; µ=3, N=24, m=3, ρ=0.95)

Fig. 1. Ratio PDF of two correlated Gamma random variables (Eq. 11) fordifferent ρ and the empirical PDF of simulatedσ0 in Gaussian clutter

Fig. 1 illustrates the behavior of theσ0 PDF with respect tothe normalized correlation coefficientρ. The PDF parametersare set according to the processing illustrated in Sect. IV,namely N = 24, m = 3, µ1 = 10, µ2 = 1. Notice thatwhen the normalized correlation coefficient approaches to1,the PDF tends to a Dirac.

A Monte Carlo simulation has been represented in Fig.1,also.5000 samples ofσ0 were obtained by computing5000×24 samplesdraw from a zero-mean multivariate circular com-plex Gaussian distribution with a covariance matrix selectedfrom the real POLSAR data. The span of the selected covari-ance matrix equal3. One can observe the good correspondencebetween the empirical PDF of simulatedσ0 and the PDFderived in Eq. 11 forρ = 0.95.

TABLE IEMPIRICAL MEAN AND VARIANCE OF THE σ0 ESTIMATOR FROMEQ. 9

AND THE THEIR EXPECTED VALUES FOR SIMULATEDGAUSSIAN CLUTTER.

Boxcar Expected EmpiricalMean Variance Mean Variance

3× 3

3 0

3.42 1.995× 5 3.13 0.517× 7 3.04 0.229× 9 3.03 0.13

Using the same parameters as in the previous Monte Carlosimulation, Table I illustrates the behavior of the empiricalmean and variance of the proposedσ0 in Gaussian clutter (e.g.in homogeneous regions). By using24 up to 48 secondarydata, the estimation bias is negligible and the empirical vari-ance is close to zero.

B. The σ0 test

In this section we propose to show how the estimator fromEq. 9 is linked with a binary hypothesis testing problem, also:

• under the null hypothesisH0, the observed target vectork =

√ξ · ζ belongs to the SIRV clutterζ ∼ N (0, [T ])

with normalized texture,• under the alternative hypothesisH1, the primary target

vector k =√

τ · z belongs to the SIRV clutterz ∼N (0, [M ]) with normalized covariance matrix.

From the operational point of view, the proposed detectoris a classical constant false alarm rate detector withcurrent pixel as primary data, and with the local boxcarneighborhood around it as secondary data.

The Neyman-Pearson optimal detector is given by thefollowing likelihood ratio test (LRT):

Λ (k) =pk(k/H1)

pk(k/H0)

H1

≷H0

λ. (12)

After expressing the PDF under each hypothesis, it results that:

Λ (k) =

1

πmdet{[M ]}τm

exp(−k

†[M ]−1k

τ

)

1

πmdet{[T ]}ξm

exp(−k†[T ]−1k

ξ

)H1

≷H0

λ. (13)

By plugging into the LRT the ML texture estimators from Eqs.5 and 8 we obtain:

Λ (k) =det{[T ]}det{[M ]}

(k†[T ]−1

k

k†[M ]−1k

)mH1

≷H0

λ. (14)

Next, we assume the ratio of determinants is a deterministicquantity and we denote it byα. This is an approximation, sincein practice the ratio of determinants is also computed usingthe ML estimators of the respective covariance matrix withNsecondary data. Finally, by replacing the known covariancesby their ML estimates the generalized LRT is:

Λ (k) = ασ0−m

H1

≷H0

λ. (15)

As α appears as a deterministic quantity only, it is possible touse the PDF derived in Sect. IV-A to set the decision thresholdλ for a specific false alarm probability.

V. RESULTS AND DISCUSSIONS

The high resolution POLSAR data set, illustrated in Fig. 2,was acquired by the ONERA RAMSES system over Toulouse,France with a mean incidence angle of500. It represents afully polarimetric (monostatic mode) X-band acquisition witha spatial resolution of approximately50 cm in range andazimuth. In the upper part of the image one can observe theCNES buildings.

Fig. 5-(a),(b),(c) presents the three SIRV parameters whichcompletely describe the POLSAR data set: the total power, thenormalized texture and the normalized covariance matrix. The5 × 5 boxcar neighborhood has been selected for illustration,hence24 secondary samples and1 primary data.

Fig. 3 presents the zoom over the red rectangle from Fig.5-(a), where a narrow diplane target was previously detected.Fig. 3-(a),(b),(c) shows the FP-PWF texture, the SCM-PWFnormalized texture, and the proposed span estimatorσ0, re-spectively. For comparison, the Multi-look PWF (MPWF) hasbeen illustrated in Fig. 3-(d). The proposed estimator exhibits

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Fig. 2. Toulouse, RAMSES POLSAR data, X-band,1500 × 2000 pixels:amplitude color composition of the target vector elementsk1-k3-k2.

better performances in terms of spatial resolution preservationthan the MPWF span estimator: the ring effect (two large dipson a spatial profile near the boundaries of a pointwise target[16]) is reduced.

Finally, Fig. 4 illustrates the detection map obtain usingthe LRT from Eq. 15 with25 secondary and one primarydata. The detection threshold has been obtained by MonteCarlo integration of the PDF from Eq. 11 with a false alarmprobability set toPfa = 10−3 in each pixel. Note thatthe PDF integration for such a small Pfa is quite timeconsuming and fast numerical approximations need to beinvestigated in the future for going to an operational level.This detection map can be interpreted as follows:

• heterogeneous clutter areas, represented in red, reveldense urban areas, which exhibit fewer dominantscatterers within the resolution cell. Over these areas,according to the hypotheses test from Sect. IV, itis better to estimate clutter parameters using thenormalized covariance SIRV model.

• homogeneous clutter areas, represented in blue, wherethe normalized texture model is better.

Concerning the validation of our results, the generalizedLRT is known to be asymptotically uniformly most pow-erful according to the Neyman-Pearson lemma [17]. This”optimality” holds provided the ML estimators pluggedinto the LRT are consistent, which is the case for ourstudy [11], [12].

VI. CONCLUSIONS

This paper presented a new estimation scheme for optimallyderiving clutter parameters with high resolution POLSARimages. The heterogeneous clutter in POLSAR data was de-scribed by the SIRV model. Three estimators were introducedfor describing the high resolution POLSAR data set: the span,the normalized texture and the speckle normalized covariancematrix. The asymptotic distribution of the new span estimatorhas been established. The estimation bias on homogeneousregions have been assessed also by Monte Carlo simulations.

Based on these issues, a novel test has been introduced forselecting the most appropriate model for POLSAR heteroge-neous clutter described by SIRVs.

This work has many interesting perspectives. We believethat this paper contributes toward the description and the anal-ysis of heterogeneous clutter over scenes exhibiting complexpolarimetric signatures. Firstly, the exact texture normalizationcondition for the PWF-SCM estimator has been derived inSect. II under the SIRV clutter hypothesis. A novel estimation/ detection strategy has been proposed which can be usedwith conventional boxcar neighborhoods directly. Finally, theproposed estimation scheme can be extended to other mul-tidimensional SAR techniques using the covariance matrixdescriptor, such as the following: repeat-pass interferometry,polarimetric interferometry, or multifrequency polarimetry.

ACKNOWLEDGMENT

The authors would like to thank Dr. S. Zozor and Dr. F.Chatelain (GIPSA-lab, France) for the very fruitful discussionsand advices. The authors would also like to thank Dr. C. Tison(CNES, France) for providing the high-resolution POLSARimages over Toulouse.

REFERENCES

[1] L. M. Novak and M. C. Burl, “Optimal speckle reduction in polarimetricSAR imagery,”IEEE Transactions on Aerospace and Electronic Systems,vol. 26, no. 2, pp. 293–305, 1990.

[2] A. Lopes and F. Sery, “Optimal speckle reduction for the product modelin multilook polarimetric SAR imagery and the Wishart distribution,”IEEE Transactions on Geoscience and Remote Sensing, vol. 35, no. 3,pp. 632–647, 1997.

[3] L. M. Novak, M. C. Burl, and W. W. Irving, “Optimal polarimetric pro-cessing for enhanced target detection,”IEEE Transactions on Aerospaceand Electronic Systems, vol. 29, no. 1, pp. 234–244, 1993.

[4] G. Liu, S. Huang, A. Torre, and F. Rubertone, “The Multilook Po-larimetric Whitening Filter (MPWF) for intensity speckle reductionin polarimetric SAR images,”IEEE Transactions on Geoscience andRemote Sensing, vol. 36, no. 3, pp. 1016–1020, 1998.

[5] G. Vasile, J.-P. Ovarlez, F. Pascal, and C. Tison, “Coherency matrixestimation of heterogeneous clutter in high resolution polarimetric SARimages,”IEEE Transactions on Geoscience and Remote Sensing, vol. 48,no. 4, pp. 1809–1826, 2010.

[6] B. Picinbono, “Spherically invariant and compound Gaussian stochasticprocesses,”IEEE Transactions on Information Theory, vol. 16, no. 1,pp. 77–79, 1970.

[7] K. Yao, “A representation theorem and its applications to spherically-invariant random processes,”IEEE Transactions on Information Theory,vol. 19, no. 5, pp. 600–608, 1973.

[8] S. Zozor and C. Vignat, “Some results on the denoising problemin the elliptically distributed context,”IEEE Transactions on SignalProcessing, vol. 58, no. 1, pp. 134–150, 2010.

[9] F. Gini and M. V. Greco, “Covariance matrix estimation for CFARdetection in correlated heavy tailed clutter,”Signal Processing, vol. 82,no. 12, pp. 1847–1859, 2002.

[10] E. Conte, A. DeMaio, and G. Ricci, “Recursive estimation of thecovariance matrix of a compound-Gaussian process and its applicationto adaptive CFAR detection,”IEEE Transactions on Image Processing,vol. 50, no. 8, pp. 1908–1915, 2002.

[11] F. Pascal, Y. Chitour, J.-P. Ovarlez, P. Forster, and P.Larzabal, “Co-variance structure maximum-likelihood estimates in compound Gaussiannoise: existence and algorithm analysis,”IEEE Transactions on SignalProcessing, vol. 56, no. 1, pp. 34–48, 2008.

[12] F. Pascal, P. Forster, J.-P. Ovarlez, and P. Larzabal, “Performanceanalysis of covariance matrix estimates in impulsive noise,” IEEETransactions on Signal Processing, vol. 56, no. 6, pp. 2206–2216, 2008.

[13] F. Chatelain, J. Y. Tourneret, and J. Inglada, “Change detection inmultisensor SAR images using bivariate gamma distributions,” IEEETransactions on Image Processing, vol. 17, no. 3, pp. 249–258, 2008.

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[14] A. Erdlyi, W. Magnus, F. Oberhettinger, and F. Tricomi,Higher Tran-scendental Functions. New York: Krieger, 1981, vol. 1.

[15] W. G. Cochran, “The distribution of quadratic forms in anormalsystem, with applications to the analysis of covariance,”MathematicalProceedings of the Cambridge Philosophical Society, vol. 30, no. 2, pp.178–191, 1934.

[16] J. S. Lee, S. R. Cloude, K. P. Papathanassiou, M. R. Grunes, and I. H.Woodhouse, “Speckle filtering and coherence estimation of polarimetricSAR interferometry data for forest applications,”IEEE Transactions onGeoscience and Remote Sensing, vol. 41, no. 10, pp. 2254–2263, 2003.

[17] L. L. Scharf, Statistical Signal Processing: Detection, Estimation, andTime Series Analysis. Addison-Wesley, Inc., 1991.

(a) (b)

(c) (d)

Fig. 3. Toulouse, RAMSES POLSAR data, X-band,50 × 50 pixels, zoomimage: (a) FP-PWF texture, (b) SCM-PWF normalized texture,(c) spanestimated usingcσ0 from Eq. 9 and (d) SCM-MPWF span.

Fig. 4. Toulouse, RAMSES POLSAR data, X-band,1500 × 2000 pixels:LRT detection map atPfa = 10−3 (SIRV with normalized texture inblueand SIRV with normalized covariance inred).

(a)

(b)

(c)

Fig. 5. Toulouse, RAMSES POLSAR data, X-band,1500×2000 pixels: (a)span estimated usingcσ0 from Eq. 9, (b) normalized textureξ, and (c) colorcomposition of the normalized coherency diagonal elements[M ]11-[M ]33-[M ]22.