I Introduction
Image pattern recognition is a common issue in medicine, biology, geography etc, in short, in domains that produce huge data in images format. Entropy, in its origins is interpreted as a disorder measure. Nevertheless, nowadays it is interpreted as the lack of information. Thus, it has been used as a methodology to measure the information content of a signal or an image. In image analysis, the greater the entropy is, the more irregular and patternless a given image is. The additive property of the standard entropy allows its use in several situations just by summing up image characteristics. Among the nonadditive entropies, we study the Tsallis entropy, which has been proposed to extent the scope of application of classical statistical physics. Here, we compare the additive BoltzmannGibbsShannon (standard) Shannon (1948) and nonadditive Tsallis entropy Tsallis (1988) when dealing with colored satellite images.
We start defining the standard entropy for black and white images and we simply extend its use to coloured images, justified by its additive property. Next, we consider the Tsallis entropy for black and white images and extend it to coloured images. Due to nonadditiveness, we call attention to some characteristics that help to qualify these images more efficiently that the standard entropy.
Ii Nonadditive entropy
Firstly, consider an black and white image with pixels. The integers and run along the and directions, respectively. Let the integer represent the image gray levels intensity of pixel . The histograms of a gray levels image are obtained by counting the number of pixels with a given intensity .
Figure 1 shows an gray scale image and the histogram produced from this image:
To properly use the entropic indexes, one must consider normalized quantities: , so that normalization condition is satisfied. The standard entropy of this image is: .
Images with low details, produce empty histograms and generate a low entropy value while images with high details produce a better filled histogram, generating high entropy values. Figure 2 illustrates the comparison:
For colored images, a given pixel has three components: red (), green () and blue (), and the integer intensity concerning each one of these colours are written as , so that . This leads to different histograms for each color: , and hence different entropies for each color: , with .
For two images and , for a given color, the entropy of the composed image, is the entropy of one image plus the other . This is the additivity property of the standard entropy, which leads to:
(1) 
Secondly, consider an black and white image mentioned before. The Tsallis entropy is for it generalizes the standard entropyTsallis (2011): , where the generalized logarithmic function is , so that, as , one retrieves the standard logarithm, consequently the standard entropy.
To build a feature vector, one simply uses different entropic values: , so that and , one retrieves the standard entropy image qualifier. Notice the richness introduced by this qualifier. If , we have already an infinity range of entropy indexes to address. This richness is amplified for , considering instances of : , and Barbieri et al. (2011).
Since , see Ref. Borges (2004), is nonadditive leading to interesting results when composing two images and . The entropy of the composed image is , which, for is not simply summation of two entropic values. This property leads to different entropic values depending on how one partitions a given image. The final image entropy is not simply to summation of the entropy of all its partitions, but it depends on the sizes of these partitions.
For colored images, we proceed as before, we calculate the entropy of each color component, in principle with different entropy indices values: , and . For sake of simplicity, we consider the same entropic index for all the color components. For color the entropy is:
(2) 
so that so that retrieves Eq. (1), for .
Iii Methodology
Considering pattern recognition in images, the main objective is to classify a given sample according to a set of classes from a database. In supervised learning, the classes are predetermined. These classes can be conceived of as a finite set, previously arrived by a human. In practice, a certain segment of data is labelled with these classifications. The classifier task is search for patterns and classify a sample as one of the database classes.
To perform this classification, classifiers usually uses a feature vector that comes from a method of data extraction. Here, we use the multi analyses method Fabbri et al. (2012) Fabbri et al. (2013) that composes a feature vector using certain entropy values: .
The reason to use the multi analysis is that a feature vector gives us more and richer information than a single value of entropy. The correct choice of indexes emphasize characteristics and provide better classifications.
The following steps describe image treatment, training and validation:

Using Google Earth software, capture images from several locations (Figure 3);

each image must be segmented in pixels partitions;

for each partition the colors Red, Green and Blue are written in a tridimensional array;

for each array and for each color, histograms are built and the Tsallis entropies (Eq. 2) are calculated, for in steps of 1/10;

the feature vector is created and the classifiers
nearest neighbors (KNN), Support Vector Machine (SVM) and BestFirst Decision Tree (BFTree) are applied;

an output image are delivered with the segmented partitions highlighted (aquatic region = yellow, urban region = cyan, vegetation regions = magenta) according with the classification of KNN classifier.
Figure 4 outlines the steps of the methodology presented:
Table 1 presents the hit rate percentage of each classifier evaluated for the 3 methods: multi analysis, multi
analysis with attribute selection and standard entropy analysis. Since the use of a feature vector gives us more information than a single entropy value it also gives some redundant information. In this context, the feature selection is important to eliminates those redundancies.
ClassifierMethod  Multi (60)  Multi * (8)  BGS (3) 

SVM  69.60  68.96  65.60 
KNN (1 neighbour)  70.80  69.76  63.04 
KNN (3 neighbours)  72.32  72.96  64.00 
KNN (5 neighbours)  72.80  73.28  64.16 
KNN (7 neighbours)  74.88  72.96  68.48 
BFTree  72.16  72.80  67.36 
*attribute selection
Figure 5 depicts image highlights produced by KNN method, evaluated in a region that contains the three types of pattern classes: aquatic, urban and vegetation regions.
Iv Conclusion
Our study indicates that the Tsallis nonadditive entropy can be successfully used in the construction of a feature vector, concerning coloured satellite images. This entropy generalizes the BoltzmannGibbs one, which can be retrieved with . For
, the image retrieval success is better that the standard case (
), once the entropic parameter allows thorougher image exploration.Acknowledgments
Lucas Assirati acknowledges the Confederation of Associations in the Private Employment Sector (CAPES) Grant . Odemir M. Bruno are grateful for São Paulo Research Foundation, grant No.: 2011/231123. Bruno also acknowledges the National Council for Scientific and Technological Development (CNPq), grant Nos. 308449/20100 and 473893/20100.
References
 Shannon (1948) C. E. Shannon, “A Mathematical Theory of Communication,” The Bell System Technical Journal, 27, 379–423–623–656 (1948).
 Tsallis (1988) C. Tsallis, “Possible generalization of BoltzmannGibbs Statistics,” Journal of Statistical Physics, 52, 479–487 (1988).
 Tsallis (2011) C. Tsallis, “The nonadditive entropy sq and its applications in physics and elsewhere: Some remarks,” Entropy, 13, 1765–1804 (2011).
 Barbieri et al. (2011) A. L. Barbieri, G. F. de Arruda, F. A. Rodrigues, O. M. Bruno, and L. da Fontoura Costa, “An entropybased approach to automatic image segmentation of satellite images,” Physica A: Statistical Mechanics and its Applications, 390, 512–518 (2011).
 Borges (2004) E. P. Borges, “A possible deformed algebra and calculus inspired in nonextensive thermostatistics,” Physica A: Statistical Mechanics and its Applications, 340, 95–101 (2004).
 Fabbri et al. (2012) R. Fabbri, W. N. Gonçalves, F. J. Lopes, and O. M. Bruno, “Multiq pattern analysis: A case study in image classification,” Physica A: Statistical Mechanics and its Applications, 391, 4487–4496 (2012).
 Fabbri et al. (2013) R. Fabbri, I. N. Bastos, F. D. M. Neto, F. J. P. Lopes, W. N. Gonçalves, and O. M. Bruno, “Multiq pattern classification of polarization curves,” arXiv, abs/1305.2876 (2013).
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