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Texture Enhancement Based on the Savitzky-Golay Fractional Differential Operator
Texture enhancement for digital images is the most important technique in image processing. The purpose of this paper is to design a texture enhancement technique using fractional order Savitzky-Golay differentiator, which leads to generalizing the Savitzky-Golay filter in the sense of the Srivastava-Owa fractional operators. By employing this generalized fractional filter, texture enhancement is introduced. Consequently, it calculates the generalized fractional order derivative of the given image using the sliding weight window over the image. Experimental results show that the operator can extract more subtle information and make the edges more prominent. In general, the capability of the generalized fractional differential will be high because it is sensitive to the subtle fluctuations of values of pixels.
Texture is an important feature of natural images; hence, a variety of image texture applications has been intensively studied by many researchers . Image texture is defined as a function of the spatial variation in pixel intensities (gray values). Smith and Chang  have defined texture as visual patterns, which have properties of homogeneity and not resulting from only a single color or intensity.
In the image, texture features capture information about repeating patterns. Texture analysis can be classified into three models: structural, statistical, and signal theoretic methods . Therefore, the analysis of texture parameters is a useful approach for increasing the information accessible from images. In texture enhancement technique, which is based on mask operation, each pixel is modified according to value of the neighbourhood around the pixel of interest. One important aspect of an image, which enables us to perform this, is the notion of frequencies. Fundamentally, the frequencies of an image are the amount, by which the gray values change with distance. High-frequency components are characterized by huge changes in gray values over small distances; examples of high frequency components are edges and noise. On the other hand, low-frequency components are parts of the image, which are characterized by little change in the gray values . Fractional differential mask can further preserve the low-frequency contour feature in those smooth areas, and nonlinearly keep the high-frequency marginal feature in those areas, where the gray-level changes heavily, and also enhances texture details in those areas, where the gray-level does not change evidently.
Fractional integration and fractional differentiation are generalizations of notions of integer-order integration and differentiation and include th derivatives and n-fold integrals as particular cases [5, 6]. Many applications of fractional calculus in physics have replaced the time derivative in an evolution equation with a derivative of fractional order [7–11]. Fractional calculus has been applied to a variety of physical phenomena, including anomalous diffusion, transmission line theory, problems involving oscillations, nanoplasmonics, solid mechanics, astrophysics, and viscoelasticity. Currently, fractional calculus (integral and differential operators) is heavily used in control design [12, 13], Furthermore, in image processing [14–19], all results that are based on the fractional calculus operators (differential and integral) show that this method not only is effective, but also has good immunity.
The digital fractional order differentiator is an important topic in fractional calculus that can estimate the fractional order derivative of any given digital signals, without known function. The Savitzky-Golay filter is a simplified digital differentiator that is implemented by a local polynomial regression technique [20, 21]. Now, Savitzky-Golay digital differentiator has been one of the most popular numerical differentiation methods, due to its high computing speed and strong antinoise ability.
Recently, the interest in using texture enhancement technique based on mask operation has grown in the field of image processing. Pu and Zhou  have implemented multiscale texture segmentation by fractional differential. They have proposed two fractional differential masks and presented the structures and parameters of each mask, respectively. Then they have discussed the multi-scale texture segmentation based on the fractional mask. Pu  has proposed a fractional calculus approach to enhance the texture of digital image. He has found that the textural detail enhancing capability of fractional derivative-based texture operator is much better than integer derivative. Zhang et al.  have used the fractional differential masks based on the classical Riemann-Liouville definition. They have concluded that the fractional order between 1 and 2 can enhance the texture and edges in multiscale, by controlling the fractional order.
In this paper, we have used a generalized fractional differential based on the generalized Savitzky-Golay filter in sense of Srivastava-Owa fractional operators for image texture enhancement. The Savitzky-Golay filter has become a powerful signal and image processing tool, which has found application in many scientific areas. Moreover, the Savitzky-Golay filter method is considered to be a good approach in image texture enhancement, which is used as an alternative to classical techniques. The rest of the paper is organized as follows: Sections 2 and 3 explain the fractional calculus and the generalized fractional integral operator, respectively, Section 4 describes the construction of fractional differential Savitzky-Golay filter, Section 5 elucidates the experimental results, and Section 6 concludes the paper.
2. Fractional Calculus
The idea of the fractional calculus (i.e., calculus of integrals and derivatives of any arbitrary real or complex order) was found over 300 years ago. Abel in 1823 scrutinized the generalized tautochrone problem and for the first time applied fractional calculus techniques in a physical problem.
2.1. The Riemann-Liouville Operators
The Riemann-Liouville fractional derivative strongly poses the physical interpretation of the initial conditions required for the initial value problems involving fractional differential equations. Moreover, this operator possesses advantages of fast convergence, high stability, and higher accuracy to derive different types of numerical algorithms .
The fractional (arbitrary) order integral of the function of order is defined by When , we write , where denoted the convolution product, , and , , and as , where is the delta function.
The fractional (arbitrary) order derivative of the function of order is defined by When , we have The Caputo fractional derivative of order is defined, for a smooth function , by where (the notation stands for the largest integer not greater than ). Note that there is a relationship between the Riemann-Liouville differential operator and the Caputo operator: and they are equivalent in a physical problem (i.e., a problem which specifies the initial conditions).
2.2. The Srivastava-Owa Operators
In , Srivastava and Owa defined and studied fractional operators (derivative and integral) in the complex -plane for analytic functions.
The fractional derivative of order is defined, for a function by where the function is analytic in simply-connected region of the complex -plane containing the origin and the multiplicity of is removed by requiring to be real when . Furthermore, for , the fractional differential operator is defined as
The fractional integral of order is defined, for a function , by where the function is analytic in simply connected region of the complex -plane () containing the origin and the multiplicity of is removed by requiring to be real when : Note that the real case of the Srivastava-Owa operators is equivalence to the Riemann-Liouville operators.
3. Generalized Fractional Integral Operator
This section briefly describes the mathematical background for the fractional integral operator that has been used by the proposed algorithm. The usual way of representing the fractional derivatives is by the Riemann-Liouville formula . Another way to represent the fractional derivatives is by the Grünwald-Letnikov formula . The discrete approximations derived from the Grünwald-Letnikov fractional derivatives present some limitations, such as the following:(i)they frequently originate unstable numerical methods;(ii)the order of accuracy of such approaches is never higher than one.
To implement the generalized fractional integral method, Ibrahim in  has imposed a formula for the generalized fractional integral. Consider, for natural and real , the -fold integral of the form Applying the Cauchy formula for iterated integrals implies Repeating the above step times we obtain which yields the fractional operator type where and are real numbers and the function is analytic in the simply connected region of the complex -plane containing the origin, and the multiplicity of is removed by requiring to be real when . When , we arrive at the standard Srivastava-Owa fractional integral, which is used to define the Srivastava-Owa fractional derivatives.
Corresponding to the generalized fractional integrals (13), we define the generalized differential operator of order by where the function is analytic in the simply connected region of the complex -plane containing the origin and the multiplicity of is removed by requiring to be real when .
Proposition 1 (see ). The generalized derivative of the function , is given by the following: which is later used to compute the coefficient matrix .
4. Construction of the Fractional Differential Savitzky-Golay Filter
The Savitzky-Golay filter has been introduced for computing the numerical derivatives and is also called a digital smoothing polynomial filter. The Savitzky-Golay method is often used to preserve higher moments in the data, thus reducing the distortion of essential features of the data.
In this section, we willgeneralize this filter for calculating the fraction derivatives which will be utilized by the proposed algorithm.
Assume a uniformly sampled signal, our aim is to estimate its th order derivative using -point filtering window and an -degree polynomial : which is used to fit the given signal . In matrix notation, (16) is reduced to the system where is the estimate error, is the coefficient matrix and is the Vandermonde matrix defined by The coefficients of the best-fit polynomial can be obtained by minimizing the sum of the squared errors between the actual data and fitting points. Thus, implies where denotes the moving window’s coefficients matrix. Consequently, the th order derivative can be estimate by
Now, in view of Proposition 1, we have where
Note that when , we have the Riemann-Liouville differential operator. Moreover, when , the Vandermonde matrix is a square matrix. The purpose of the Savitzky-Golay filter is to estimate , which can be used to calculate the th order derivative of any given signal . The coefficient matrix can be computed by where where is the sampling interval.
The matrix can be assumed as the formula of computation time; therefore, the generalized Savitzky-Golay filter can be viewed as the generalization of the differentiator. However, digital image is a function of two variables, so, we can generalize these definitions to include both the and values.
The mask is designed into size matrix which has layers ( is odd). The window’s size can be an arbitrary odd number, and a larger window can improve the accuracy of fractional differential, but increases the computational time. Therefore, we proceed to use moving window with size as shown in Table 1.
The fractional differential operator can enhance edges and contours as well as reserve the texture details. The nine values output of each fractional differential window is performed by sliding the mask window over the image . Generally one can start at the top left corner of the image block through all the pixels, where the fractional differential mask fits entirely within the boundaries of the image. The output of each image block is nine values, which represent the texture information in each image block, that takes the following formula: where is the value of an image pixel and is the value of filter mask.
5. Experimental Results and Discussion
The reason of this experiment is to validate the correctness of the proposed algorithm.
Performance tests for the algorithm proposed by this paper were implemented using Matlab 2010a on Intel (R) Core i7 at 2.2 GHz, 4 GB DDR3 Memory, and system type 64-bit, Window 7. The computation time per image differs for each image and depends mainly on the window’s size as well as image size.
The proposed texture features enhancement algorithm includes the following steps:(i)read the original gray-scale image;(ii)set the value of and (≥1);(iii)set the value of the image sampling interval ;(iv)set the values of the fractional power parameters ();(v)compute Savitzky-Golay moving window as in (24);(vi)compute the Vandermonde matrix as in (25);(vii)apply the Savitzky-Golay fractional differential mask with the corresponding image pixels by sliding the window over the image.
Tables 2 and 3. show the coefficients of the fractional differential moving window for different values of . All coefficient values are not equal to zero, which implies that the magnitude response of Savitzky-Golay filter is not also zero in the image region. This will likelyimprove the texture detail. However, the qualities of texture is defined by the spatial distribution of gray values for this reason, we have used gray-scale images for testing, which are shown in Figures 1(a) and 1(b).
The proposed enhancement algorithm shows good enhancement performance for both, testing images by different degrees of fractional power values and which are experimentally fixed at , 0.5 and , and the value of the image sampling interval . It is seen that, the proposed enhancement algorithm using fractional differential masks, can extract more texture information and sharpen edges more efficiently. The eye’s qualitative analysis of the proposed algorithm acts as one of the important parameters to judge its performance.
Other metrics used to judge the algorithm performance are the statistical measures. In this paper, among the statistical features, the following second-order statistics are used as texture features in representing images. The gray-level co-occurrence matrix (GLCM) is a statistical method used to describe textures in an image, by modeling texture as a two-dimensional gray level variation . Four statistical measures are extracted to evaluate the images texture enhancement; these are entropy, homogeneity, contrast, and energy.(1) Entropy measures the amount of information, and the larger value of entropy is the greater amount of information carried by image, but inversely correlated to energy. Entropy feature of gray-scale cooccurrence matrix is one of the features having the best discriminatory power, which is given in following equation: where is the probability for gray-scale and and occurs at two pixels.(2) Homogeneity measures the closeness of the distribution of elements in the GLCM to the GLCM diagonal: (3) Contrast measures the intensity contrast between a pixel and its neighbour over the whole image: (4) Energy measures the sum of squared elements in the gray-level cooccurrence matrix (GLCM):
Figure 2 shows the results of the proposed enhancement algorithm for with (a) , and (b) . The variation of the image texture is observed when is increased from 0.4 to 0.5. So, the selection of differential order is important.
Tables 4 and 5 and Figures 3 and 4 show the performance evaluation of the proposed algorithm for image (a) and image (b) according to those four statistical measures of gray-level cooccurrence matrix (GLCM). It can be clearly seen that there has been a large increase in the value of entropy, which means the greater amount of information is carried by image due to texture enhancement. The entropy values for image (a) climbed to approximately 0.224 for and to 0.26 for for all texture enhancement cases. Moreover, for image (a), it inversely correlated to energy, which decreases to approximately 0.881 for and to 0.860 for and from its value of the original testing image. The homogeneity steadiness is reduced with the increase of texture enhancement, which means more divergence of the distribution of elements of information carried by image due to texture enhancement process. While the contrast showed diverse tendencies for all texture enhancement cases, it is conclude that the intensity contrast between a pixel and its neighbour over the whole image are changed too. This variation in the statistical measures makes the proposed algorithm capable to control the degree of texture enhancement of the image by controlling the fractional order parameters and .
In this paper, a texture enhancement technique using fractional order Savitzky-Golay differentiator, which leads to generalize Savitzky-Golay filter in sense of Srivastava-Owa fractional operators, have been introduced. The new algorithm presented in this paper can control the degree of texture enhancement of the image with the fractional power values. The new approach can control the degree of texture enhancement of the image with fractional order of the parameters , and . However, the technique is by no means limited only to images, instead, it can be applied in the setting of different image applications, taking into consideration the limitations of each imaging method. Furthermore, our goal is to keep away from the effect of the noise that caused in the texture enhancement of the image and to control the degree of texture enhancement of the image with the filter mask parameters. The experiment results had demonstrated the efficacy of this algorithm according to the metrics used to judge the algorithm performance.
The authors would like to thank the reviewers for their comments on earlier versions of this paper. This research has been funded by university of Malaya, under Grant no. UMRG 104-12ICT.
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Copyright © 2013 Hamid A. Jalab and Rabha W. Ibrahim. 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.