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Journal of Probability and Statistics

Volume 2013 (2013), Article ID 170967, 13 pages

http://dx.doi.org/10.1155/2013/170967

## Masses of Negative Multinomial Distributions: Application to Polarimetric Image Processing

^{1}Université de Pau et des Pays de l'Adour, Avenue de l'Université, 64012 Pau, France^{2}Gipsa-Lab, Département Images et Signal, 961 rue de la Houille Blanche, BP 46, 38402 Saint Martin d'Héres, France^{3}Université de Toulouse, IRIT/ENSEEIHT/TESA, 2 rue Charles Camichel, BP 7122, 31071 Toulouse Cedex 7, France

Received 5 June 2012; Revised 30 October 2012; Accepted 8 November 2012

Academic Editor: Edwin Ortega

Copyright © 2013 Philippe Bernardoff et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

This paper derives new closed-form expressions for the masses of negative multinomial distributions. These masses can be maximized to determine the maximum likelihood estimator of its unknown parameters. An application to polarimetric image processing is investigated. We study the maximum likelihood estimators of the polarization degree of polarimetric images using different combinations of images.

#### 1. Introduction

The univariate negative binomial distribution is uniquely defined in many statistical textbooks. However, extensions defining multivariate negative multinomial distributions (NMDs) are more controversial. Most definitions are based on the probability generating function (PGF) of these distributions. Doss [1] proposed to define the PGF of an NMD as the inverse th power of a polynomial linear in each of its variables. This definition can also be found in the famous textbook [2, page 93] and the computation of its modes has been investigated in [3]. A more general class of NMDs introduced in [4] was characterized by PGFs of the form , where , is an matrix, and . In particular, matrices yielding infinitely divisible PGFs were derived. Finally, Bar-Lev et al. [5] introduced NMDs whose PGFs are defined as the inverse th power of any affine polynomial. Necessary and sufficient conditions on the coefficients of this affine polynomial were derived to obtain the PGF of a multivariate distribution defined on (where is the set of nonnegative integers) [6]. These very general multivariate NMDs were recently used for image processing applications in [7].

The family of NMDs introduced in [5] can be defined as follows. Let us denote the set of the first nonzero integers. We denote as the monomial obtained by multiplying all the entries of the vector whose indexes belong to , where stands for any subset of the indexes. Let be an affine polynomial with respect to the variables such that . The NMD distribution defined at pair is represented by its PFG which is given by Such laws are denoted as . However, as explained in [6], all couples do not provide a valid NMD. More specifically, Bernardoff has derived a finite number of conditions over such that is the PGF of an NMD for all positive integer . The corresponding expression of the coefficient of in the Taylor expansion of is given by the formula where and is the set of all subsets of . However, this expression of does not allow us to explicitly compute the masses of NMDs in the general case.

As a first goal of this paper, we propose a way of computing the masses of multivariate NMDs defined above. A specific attention is devoted to bivariate and trivariate cases. In particular, it allows us to retrieve the results of [7] obtained for bivariate NMDs. The second part of the paper is devoted to the application of NMDs to image processing, more specifically to polarimetric image processing [8, 9]. Polarimetric image processing has received a considerable attention in the image processing and optical communities (see for instance [10–12] and references therein). The state of polarization of a polarimetric image is classically characterized by the degree of polarization (DoP) whose estimation is of major importance [13, 14]. The DoP of polarimetric images can be classically estimated by using four images associated to four different polarizations [15]. However, estimating the DoP using less than four images is interesting since it allows one to reduce the acquisition time and the resulting cost of the imaging system. As a consequence, there has been recently an increasing interest in deriving estimators of the DoP based on a reduced number of polarimetric images. Depending on the intensity of the acquired images, polarimetric images are referred to as low flux or high flux images (low flux corresponding to a small intensity and high flux to a larger intensity). DoP estimation based on a single polarimetric image was considered in [16, 17] under high flux and low flux assumptions. DoP estimators derived from two intensity images degraded by fully developed speckle noise were studied in [18, 19]. Finally, imaging systems using three polarimetric images were studied in [20, 21], under high flux and low flux assumptions.

This paper studies the maximum likelihood estimators (MLEs) of the square DoP based on two or three polarimetric images. These estimators are computed by maximizing the masses of bivariate or trivariate NMDs derived in the first part of this work.

The paper is organized as follows. Section 2 recalls important results on NMDs. Section 3 proposes a new way of computing masses of NMDs. A particular attention is devoted to bivariate and trivariate cases. Section 4 addresses the problem of estimating the square DoP of low flux polarimetric images using the maximum likelihood (ML) principle. Different MLEs are constructed depending on the number of available polarimetric images. Simulation results are presented in Section 5.

#### 2. Negative Multinomial Distributions

An -variate NMD is the distribution of a random vector taking its values in whose PGF is where denotes the mathematical expectation, , and is an affine polynomial of order . (A polynomial with respect to is affine if the one variable polynomial can be written as (for any ), where and are polynomials with respect to the 's with .) These discrete distributions have received much interest in the literature (see for instance [2] and the references therein). Of course, the affine polynomial has to satisfy appropriate conditions to ensure that is a PGF. These conditions include the trivial equality . However, determining all pairs such that is a PGF is still an open problem (see [6], for discussions related to this problem). As explained in [6], the affine polynomial can be rewritten where are positive numbers and is an affine polynomial such that . The Taylor expansions of and in the neighborhood of will be denoted as follows: where and . Equations (3) and (4) clearly show that the masses of multivariate NMDs denoted as can be expressed as follows:

#### 3. Masses of Negative Multinomial Distributions

In this section, we derive new expressions for the coefficients that will be used to compute the masses of NMDs. The particular cases of bivariate and trivariate NMDs will play an important role for the estimation of the DoP on polarimetric images. In order to compute the , we derive several results summarized in this section whereas all demonstrations are reported in the appendix.

Theorem 1. *Denote as the set of nonempty subsets of . Any affine polynomial such that denoted as
**
can be expressed as follows:
**
where is the cardinal of the set . Moreover
**
where is the polynomial defined by and is related to the variables as follows:
*

*Remark 2. * In the trivariate case defined by , the polynomial can be expressed as
where the coefficients of the polynomial
can be determined using the relations
The next theorem provides a relation between the coefficients of the polynomials and introduced above.

Theorem 3. *Let , , and be the affine polynomial defined in (10) and (11). For any and in , denote as the coefficient of in the Taylor expansion of and as the coefficient of in the Taylor expansion . The following relation can be obtained:*

The masses of NMDs can be directly obtained from this theorem. The particular cases of bivariate and trivariate NMDs are considered in the following subsections since the corresponding masses will be useful in the application considered in the second part of this paper.

##### 3.1. Bivariate NMDs

Theorem 4. * Consider the affine polynomial of order 2 with variables defined by
**
The coefficient of in the Taylor expansion of , can be computed as follows
*

*Remark 2. *The result was mentioned in [7] without the factorization leading to (19). If and , an equivalent formulation of (19) is

##### 3.2. Trivariate NMDs

Theorem 6. * Consider the affine polynomial with the three variables defined by
**
The coefficient of in the Taylor expansion of are
**
When , , , , , and , an equivalent expression is
*

#### 4. Estimating the Polarization Degree of Low Flux Polarimetric Images Using Maximum Likelihood Methods

##### 4.1. Low Flux Polarimetric Images

The state of the polarization of the light can be described by the random behavior of a complex vector , called the Jones vector, whose covariance matrix, called the polarization matrix, is where* denotes the complex conjugate. The covariance matrix is a nonnegative Hermitian matrix whose diagonal terms are the intensity components in the and directions. The cross terms of are the correlations between the Jones components. If we assume a fully developed speckle, the Jones vector is distributed according to a complex Gaussian distribution whose probability density function (pdf) is [15]: where is the determinant of the matrix and denotes the conjugate transpose operator. As a consequence, the statistical properties of are fully characterized by the covariance matrix . The different components of can be classically estimated by using four intensity images that are related to the components of the Jones vector as follows (see [20], for more details): The state of the polarization of the light is classically characterized by the square DoP defined by [15, pages 134–136] where is the trace of the matrix . The light is totally depolarized for , totally polarized for , and partially polarized when . As a consequence, estimating the square DoP of a polarimetric image is important in many practical applications. Different estimation methods of using several combinations of intensity images were studied in [20]. Since only one realization of the random vector was available for a given pixel of a polarimetric image, the image was supposed to be locally stationary and ergodic. These assumptions were used to derive square DoP estimators using several neighbor pixels belonging to a so-called estimation window.

This paper considers practical applications where the intensity level of the reflected light is very low (low flux assumption), which leads to an additional source of fluctuations on the detected signal. Under the low flux assumption, the quantum nature of the light leads to a Poisson-distributed noise which can become very important relatively to the mean value of the signal at a low photon level. As a consequence, the observed pixels of the low flux polarimetric image are discrete random variables contained in the vector such that the conditional distributions of the random variables , for are independent and distributed according to Poisson distributions with means , for . The resulting joint distribution of is a multivariate mixed Poisson distribution [22]: where , , and is the joint pdf of the intensity vector. This section studies estimators of the square DoP defined in (28) based on several vectors belonging to the estimation window. These estimators are constructed from estimates of the covariance matrix elements , . As explained in the introduction, several studies have been recently devoted to the estimation of the square DoP using less than four polarimetric images. This paper goes into this direction by deriving estimators based on the observation of 2 or 3 polarimetric images.

The joint distribution of the intensity vector is known to be a multivariate gamma distribution whose Laplace transform is [20] where the affine polynomial is with and As a consequence, the distribution of is an NMD whose PGF can be written as (the interested reader is invited to consult [22] for more details) The results of Section 2 allow us to compute the masses of that will be useful for studying the maximum likelihood estimator (MLE) of the square DoP.

##### 4.2. MLE Using Three Polarimetric Images

The PGF of can be computed from (33) by setting . The following result can be obtained: with , and . The results of Section 3.2 can then be used to express the masses of as a function of .

The ML estimator of based on several vectors belonging to the estimation window (where and is the number of pixels of the observation window) is obtained by maximizing the log-likelihood with respect to (note again that is the mass of a trivariate NMD that has been computed in Section 3.2). The practical determination of the ML estimator of is achieved by using a Newton-Raphson procedure. The ML estimators of the vector , denoted as , are then plugged into (28) to provide the ML estimator of the square DoP based on three polarimetric images:

##### 4.3. MLE Using Two Polarimetric Images

The PGF of can be computed from (34) by setting . The following result can be obtained: with and . The results of Section 3.1 can then be used to express the masses of as a function of .

The MLE of based on several vectors belonging to the estimation window is obtained by maximizing the log-likelihood with respect to (note that is the mass of a bivariate NMD that has been computed in Section 3.1). The practical determination of the ML estimator of is achieved by using a Newton-Raphson procedure. The ML estimators of the vector elements, denoted as , are then plugged into (28) to provide the MLE of the square DoP based on two polarimetric images:

#### 5. Simulation Results

##### 5.1. Estimation Performance

The performance of the ML estimators of the square DoP based on two or three polarimetric images has been evaluated via several experiments. The first simulations compare the log Mean Square Errors (MSEs) of the square DoP estimators constructed from two or three images. Eleven different covariance matrices of the Jones vector have been considered in order to define typical values of the DoP. The values of , for , (defining the covariance matrix elements of the Jones vector) and the corresponding values of the square DoPs are reported in Table 1. Note that all the covariance matrices , , have been normalized so that the mean of the total intensity is equal to 4. Thus, the average number of photons collected on each pixel equals 4 for each matrix of the considered set. This point is in agreement with the low flux assumption.

Figure 1(a) display the empirical log MSEs of the square DoP estimators for the set of covariance matrices defined in Table 1 as a function of the true square DoP value. The red plus markers + correspond to the estimators obtained for two polarimetric images (2D MLE), whereas the blue cross markers × correspond to the MLE obtained for three polarimetric images (3D MLE). Note that these empirical MSEs have been computed for a square observation window of size pixels, based on Monte-Carlo runs. The theoretical asymptotic log MSEs of the MLE are also displayed in Figure 1(a) with continuous lines. These asymptotic values correspond to the Cramer-Rao Lower Bound (CRLB) for the parameter . The MLE is known to be asymptotically unbiased and efficient under mild regularity conditions (that are satisfied for ). Thus, the MSE of the estimates can be approximated a for large sample by the CRLB. More details about the way of computing the square DoP CLRBs can be found in [23]. Figure 1(a) indicates that the empirical MSEs are in good agreement with the corresponding CRLBs, except for the matrices and . Indeed, the CRLBs for these two matrices cannot be computed since the true value of the parameters belongs to the boundary of its definition domain. The empirical bias, standard deviations (“std”), MSEs, and asymptotic variances (“avar”) of the estimators of are also reported in Table 2. It is interesting to note that the MLE obtained using 3 images is slightly more biased than the one obtained using 2 images. However, the MLE based on 3 images provides lower MSEs than the estimator based on 2 images, as expected.

In order to appreciate the influence of the Poisson noise due to the low flux assumption, experiments have been conducted using the high flux assumption. In this case, the intensity vector is assumed to be known. Thus, the high flux MLEs using two and three images can be derived from the intensity vectors and [20]. The results are depicted in Figure 1(b). A comparison between Figures 1(a) and 1(b) allows one to appreciate a similar global behaviour for all the estimators, with a maximum MSE near and decreasing MSEs as goes to or . The degradation of the estimation performance due to the presence of Poisson noise (due to the low flux assumption) can also be clearly noticed.

The next set of simulations studies the performance of the different estimators as a function of the sample size . Figures 2(a) and 2(b) show the log MSEs of the square DoP estimates obtained for and images (for the two particular matrices and ). The empirical bias, standard deviations (“std”), MSEs, and asymptotic variances (“avar”) are also reported in Tables 3 and 4. One can see that the empirical MSEs are in good agreement with their theoretical asymptotic values for a large enough sample size, that is, . Moreover, the gain of a performance using images instead of is more significant for small values of (indeed, the difference between the different curves is more pronounced in the left figure corresponding to than in the right figure corresponding to .)

Figures 3(a) and 3(b) display the MSEs of the MLE under the high flux assumption. By comparing Figures 2 and 3, one can observe that the gain of performance using images instead of is more important in the high flux scenario than under a low flux assumption.

##### 5.2. Application to Synthetic Polarimetric Images

In order to appreciate the estimation performance on polarimetric images, we consider a synthetic polarimetric image of size composed of three distinct objects located on a homogeneous background depicted in Figure 4 (see also [20]). The polarimetric properties of these objects and background (i.e., the covariance matrix of the Jones vector and the square DoPs) are reported in Table 5. The polarimetric low flux images generated according to this model are also represented in Figure 5 in negative colors (bright pixels correspond to a small number of photons, dark ones correspond to a large number of photons). Note that these images represent the values of the vector for each pixel. The square DoP of each pixel (for ) has been estimated from vectors belonging to windows of size centered around the pixel of coordinates in the analyzed image. The estimated square DoPs are depicted in Figures 6(a) and 6(b) for the MLEs using 2 and 3 images, respectively. One can see that the ML method for 3 images gives more homogeneous results on each object than the ML method derived for 2 images. This result confirms that the MLE using 3 images performs better than the MLE using only 2 images. However, the polarimetric properties of a scene can be clearly recovered with 2 or 3 low flux images.

##### 5.3. Estimation Results on Real-Word Polarimetric Images

Finally, the ML estimator based on three images is applied on real polarimetric data. These images are acquired by using a laser as a coherent illumination source. The scene consists of two disks. The first one, intended to provide low DoP, is a grey diffuse material (left object in Figure 7). The second one is made of sand blasted aluminium providing high DoP (right object in Figure 7). Due to the experimental conditions, the measured intensities are quite low. As a consequence, these intensities are assumed to be distributed according to an NMD. The intensity images corresponding to , , , and are depicted in Figure 7. The interested reader is invited to read [20] for more details on these data. It is important to note that the two disks exhibit the similar level of total reflectivity and can hardly be distinguished without a polarimetric processing.

Figure 8 shows the ML estimates of the square DoPs for images and an estimation window of size pixels. As expected, the values of the estimates are quite different on each disk: quite higher on the metal than on the plastic disk. This result is in good agreement with the theoretical properties of the considered material. This emphasizes the interest in considering efficient estimators based on NMDs for polarimetric images.

#### Appendix

#### Proofs of the Theorems

*Proof of Theorem 1. *The set of affine polynomials with real coefficients and variables is a vector space of dimension spanned by the basis . The set of polynomials is another basis of this vector space. The proof of the theorem is obtained by expressing the coefficients of in this latter basis. Considering the expansion
the following results can be obtained.(1)Substituting in (A.1) leads to .(2)Substituting in (A.1), where if and else leads to
or equivalently
(3)Without loss of generality, if , the coefficients can be computed for . Indeed, consider a permutation such that . If , we have . Using the relation
the expansion
yields for any ,
In order to determine , we can assume , and substitute , in (A.5). The following result is obtained
hence

*Proof of Theorem 3. *The relation (10) leads to
which proves (15). Straightforward computations allow us to obtain the equalities (16) and (17) from (15).

*Proof of Theorem 4. *Denote , and introduce the notation of [6]
where . By using Theorem 3, the following results can be obtained

*Proof of Theorem 6. *The relation (16) with leads to (22). By using the trivial equality
we easily obtain (23). Note that for , we have . By substituting , in (23), the last result (24) can be obtained.

#### Acknowledgments

The authors would like to thank Gérard Letac for fruitful discussions regarding multivariate gamma distributions and negative multinomial distributions. The Authors are also grateful to Mehdi Alouini for acquiring and providing them the polarimetric images.

#### References

- D. C. Doss, “Definition and characterization of multivariate negative binomial distribution,”
*Journal of Multivariate Analysis*, vol. 9, no. 3, pp. 460–464, 1979. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at Scopus - N. L. Johnson, S. Kotz, and N. Balakrishnan,
*Discrete Multivariate Distributions*, John Wiley & Sons, New York, NY, USA, 1997. - F. Le Gall, “The modes of a negative multinomial distribution,”
*Statistics and Probability Letters*, vol. 76, no. 6, pp. 619–624, 2006. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at Scopus - R. C. Griffiths and R. K. Milne, “A class of infinitely divisible multivariate negative binomial distributions,”
*Journal of Multivariate Analysis*, vol. 22, no. 1, pp. 13–23, 1987. View at Zentralblatt MATH · View at Scopus - S. K. Bar-Lev, D. Bshouty, P. Enis, G. Letac, I. L. Lu, and D. Richards, “The diagnonal multivariate natural exponential families and their classification,”
*Journal of Theoretical Probability*, vol. 7, no. 4, pp. 883–929, 1994. View at Publisher · View at Google Scholar · View at Scopus - P. Bernardoff, “Which negative multinomial distributions are infinitely divisible?”
*Bernoulli*, vol. 9, no. 5, pp. 877–893, 2003. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at Scopus - F. Chatelain, S. Lambert-Lacroix, and J. Y. Tourneret, “Pairwise likelihood estimation for multivariate mixed Poisson models generated by gamma intensities,”
*Statistics and Computing*, vol. 19, no. 3, pp. 283–301, 2009. View at Publisher · View at Google Scholar · View at Scopus - C. Brosseau,
*Fundamentals of Polarized Light—A Statistical Approach*, John Wiley & Sons, New York, NY, USA, 1998. - J. S. Lee and E. Pottier,
*Polarimetric Radar Imaging: From Basics to Applications*, Optical Science and Engineering, Taylor & Francis, London, UK, 2009. - S. Huard,
*Polarization of LightStatistical Optics*, John Wiley & Sons, New York, NY, USA, 1997. - H. Mott,
*Remote Sensing With Polarimetric Radar*, John Wiley & Sons, New York, NY, USA, 2007. - R. Shirvani, M. Chabert, and J. Y. Tourneret, “Ship and oil-spill detection using the degree of polarization in linear and hybrid/compact dual-pol SAR,”
*IEEE Journal of Selected Topics in Applied Earth Observations and Remote Sensing*, vol. 5, no. 3, pp. 885–892, 2012. View at Publisher · View at Google Scholar - R. C. Jones, “A new calculus for the treatment of optical systems V. A more general formulation and description of another calculus,” vol. 37, no. 2, pp. 107–110, 1947. View at Publisher · View at Google Scholar
- E. Wolf, “Coherence properties of partially polarized electromagnetic radiation,”
*Il Nuovo Cimento*, vol. 13, no. 6, pp. 1165–1181, 1959. View at Publisher · View at Google Scholar · View at Zentralblatt MATH · View at Scopus - J. Goodman,
*Statistical Optics*, John Wiley & Sons, New York, NY, USA, 1985. - J. Fade, M. Roche, and P. Réfrégier, “Precision of moment-based estimation of the degree of polarization in coherent imagery without polarization device,”
*Journal of the Optical Society of America A*, vol. 25, no. 2, pp. 483–492, 2008. View at Publisher · View at Google Scholar · View at Scopus - J. Fade, P. Réfrégier, and M. Roche, “Estimation of the degree of polarization from a single speckle intensity image with photon noise,”
*Journal of Optics A*, vol. 10, no. 11, Article ID 115301, 2008. View at Publisher · View at Google Scholar · View at Scopus - P. Réfrégier, M. Roche, and F. Goudail, “Cramer-Rao lower bound for the estimation of the degree of polarization in active coherent imagery at low photon levels,”
*Optics Letters*, vol. 31, no. 24, pp. 3565–3567, 2006. View at Publisher · View at Google Scholar · View at Scopus - M. Roche, J. Fade, and P. Réfrégier, “Parametric estimation of the square degree of polarization from two intensity images degraded by fully developed speckle noise,”
*Journal of the Optical Society of America A*, vol. 24, no. 9, pp. 2719–2727, 2007. View at Publisher · View at Google Scholar · View at Scopus - F. Chatelain, J. Y. Tourneret, M. Roche, and M. Alouini, “Estimating the polarization degree of polarimetric images in coherent illumination using maximum likelihood methods,”
*Journal of the Optical Society of America A*, vol. 26, no. 6, pp. 1348–1359, 2009. View at Publisher · View at Google Scholar · View at Scopus - W. B. Sparks and D. J. Axon, “Panoramic polarimetry data analysis,”
*Publications of the Astronomical Society of the Pacific*, vol. 111, no. 764, pp. 1298–1315, 1999. View at Publisher · View at Google Scholar · View at Scopus - A. Ferrari, G. Letac, and J. Y. Tourneret, “Multivariate mixed poisson distributions,” in
*Proceedings of the EUSIPCO-04*, F. Hlawatsch, G. Matz, M. Rupp, and B. Wistawel, Eds., pp. 1067–1070, Vienna, Austria, September 2004. - F. Chatelain,
*Lois statistiques multivariees pour le traitement de l'image [Ph.D. thesis]*, Institut National Polytechnique de Toulouse, Toulouse, France, 2007.