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SURVEY OF SUPERRESOLUTION USING PHASED BASED IMAGE MATCHING

Superresolution (SR) is a method of enhancing image resolution by combining information from multiple images. Two main processes in superresolution are registration and image reconstruction. Both of these processes greatly affect the quality image of the superresolution. Accurate registration is required to obtain high-resolution image quality. This research propose a collaboration between Phase-Based Image Matching (PBIM) registration, and reconstruction using Structure-Adaptive Normalized convolution algorithm (SANC) and Projection Onto Convex sets algorithm (POCs). PBIM was used to estimate translational registration stage. We used the function fitting around the peak point, to obtain sub pixel accurate shift. The results of this registration were used for reconstruction. Three registration method and two reconstruction algorithms have been tested to obtain the most appropriate collaboration by measuring the value of Peak Signal to Noise Ratio (PSNR). The result showed that the collaboration of PBIM and both reconstruction algorithm, SR with PBIM and POCs have PSNR average of 32.12205, while PSNR average of SR with SANC algorithm was 32.07325. For every collaborative algorithms that have been tested, registration PBIM with function fitting, has an higher average PSNR value than the Keren and Marcel registration.

Journal of Theoretical and Applied Information Technology 30th September 2012. Vol. 43 No.2 © 2005 - 2012 JATIT & LLS. All rights reserved. ISSN: 1992-8645 www.jatit.org E-ISSN: 1817-3195 SURVEY OF SUPERRESOLUTION USING PHASED BASED IMAGE MATCHING 1 BUDI SETIYONO, 2MOCHAMAD HARIADI, 2MAURIDHI HERY PURNOMO Department of Mathematics Sepuluh Nopember Institute of Technology, Surabaya – Indonesia 2 Department of Electrical Engineering Sepuluh Nopember Institute of Technology, Surabaya – Indonesia E-mail: 1masbudisetiyono@gmail.com, 2mochar@gmail.com, 2hery@ee.its.ac.id 1 ABSTRACT Superresolution (SR) is a method of enhancing image resolution by combining information from multiple images. Two main processes in superresolution are registration and image reconstruction. Both of these processes greatly affect the quality image of the superresolution. Accurate registration is required to obtain high-resolution image quality. This research propose a collaboration between Phase-Based Image Matching (PBIM) registration, and reconstruction using Structure - Adaptive Normalized convolution algorithm (SANC) and Projection Onto Convex sets algorithm (POCs). PBIM was used to estimate translational registration stage. We used the function fitting around the peak point, to obtain sub pixel accurate shift. The results of this registration were used for reconstruction. Three registration method and two reconstruction algorithms have been tested to obtain the most appropriate collaboration by measuring the value of Peak Signal to Noise Ratio (PSNR). The result showed that the collaboration of PBIM and both reconstruction algorithm, SR with PBIM and POCs have PSNR average of 32.12205, while PSNR average of SR with SANC algorithm was 32.07325. For every collaborative algorithms that have been tested, registration PBIM with function fitting, has an higher average PSNR value than the Keren and Marcel registration. Keywords: Phased Based Image Matching, Reconstruction, Registration, Superresolution, SANC, POCs 1. INTRODUCTION Data or information is not only expressed in the form of text, but also may include multimedia as images, audio, and video. Image as one of the multimedia component holds very important role as a form of visual information. The higher resolution image provide more detailed information. Image with high resolution can be obtained by improving the quality of the CCD, but it is costly. Another approach is the superresolution. It is done by processing the signal, that require lower cost. Superresolution (SR) is a method to improve the resolution of Low Resolution images (LR) into High Resolution image (HR). Based on the number of reference images are used, superresolution can be grouped into two categories. They are superresolution using an image, and superresolution using multiple images in the same scene as reference [1]. Some researches showed that the good reconstructions were strongly influenced by the registration process [1][2][3]. Phase Based Image Matching (PBIM) was used to estimate the translational registration stage, because of its high accuracy up to 0.01 pixel. Only translation with sub pixel accuracy that contributed in the reconstruction process[4][5][6]. The research also showed that PBIM was better in performance, efficiency and complexity compared to the block-matching method. Other researchers compared two registration techniques, algorithms based on nonlinear optimization and Discrete Fourier transform (DFTs). The results showed that after being compared with usual FFT approach, these algorithms have shorter computational time and also required less memory[7][8] Several popular and powerful reconstruction algorithms that have been developed are the Structure-Adaptive Normalized convolution SANC[9][10]. The Structure-Adaptive Normalized convolution (SANC) algorithm is the image interpolation algorithms that work on the scope of Normalized convolution. This algorithm defines the applicable function based on the distance to the neighboring pixel point. Other reconstruction algorithm is the Projection Onto Convex Sets (POCs). The algorithm is effective for the reconstruction of image containing motion blur and has noise [11][12]. Several studies related to the superresolution have been conducted by researchers.[13][14][15][16][17]. 245 Journal of Theoretical and Applied Information Technology 30th September 2012. Vol. 43 No.2 © 2005 - 2012 JATIT & LLS. All rights reserved. ISSN: 1992-8645 www.jatit.org In this research authors conducted a collaborative study between the registration and reconstruction process. The registration process used PBIM, while the reconstruction used two algorithm, such as SANC and POCs to find the best performance in producing high-resolution image. We fitted the data points around the peak point, to obtain more accurate shifting of the sub pixel. Block diagram in Figure 1 is the stages that performed in this research. In this study, superresolution began with taking objects using video. They were extracted to obtain a series of images in the same scene.. Then pixels translation was estimated using Phased Based Image Matching and fitted for the sub-pixel level shifting. In determining the effect of registration and reconstruction of objects which have different characteristics, we used some images that contain lots of texture and some other with less texture for experiment. The authors also compared the accuracy of the PBIM registration with fitting and Keren and Marcel registration. The registration results were used for reconstruction using SANC and POCs algorithm This paper is organised as follows. Section 2 presents the problems related to superresolution and techniques registration using PBIM, and the fitting function to estimate the level of sub-pixel shifting. Section 3 presents a reconstruction algorithm using the SANC and POCs algorithm. Furthermore, section 4 describes the result and the discussion of collaboration between the registration and reconstruction. Finally, section 5 is a conclusion. E-ISSN: 1817-3195 Figure 1. Block Diagram of Research 2.1. Phased Based Image Matching 2. SUPERRESOLUTION Suppose there are two images Superresolution has two main stages, which are the registration and reconstruction. The registration is done by estimating the pixels translation, which is useful for reconstruction. If the translation pixels is in integer, then each image will contain the same information. This cannot be used in superresolution. But if the translation level are in real pixels (sub pixels), it will obtain additional information that will be useful at the time of reconstruction. Figure 2 shows the step of the superresolution. In this research, authors conducted collaboration between registration with PBIM and two reconstruction algorithms, Structure-Adaptive Normalized Convolution (SANC) and the Projection onto Convex Sets (POCs) algorithm. f (n1 , n2 ) and g (n1 , n2 ) with dimensions N1 × N 2 . Assumed index n1 ranged from − M 1 ,...,M 1 and n2 ranged from − M 2 ,...,M 2 . To simplify these indexes we used the equations N1 = 2M 1 + 1 and N 2 = 2M 2 + 1 . Discrete Fourier transform of image is : F (k1 , k 2 ) = ∑ f (n1 , n2 )W Nk11n1W Nk22n2 (1) n1n2 = AF ( k1 , k 2 )e jθ F ( k1 , k 2 ) G (k1 , k 2 ) = ∑ g (n1 , n2 )W Nk11n1W Nk22n2 (2) n1n2 = AG (k1 , k 2 )e jθ G ( k1 , k2 ) 246 Journal of Theoretical and Applied Information Technology 30th September 2012. Vol. 43 No.2 © 2005 - 2012 JATIT & LLS. All rights reserved. ISSN: 1992-8645 www.jatit.org E-ISSN: 1817-3195 M1 ∑ • operator show • WN1 = e 2π N1 ∑ ∑ n1 = − M 1 n2 = − M 2 n1n2 j M2 j , WN 2 = e 2π N2 • j is imaginer component ∧ R (k1 , k 2 ) defined in Cross spectrum phase equation (3) as ∧ R (k1 , k 2 ) = F (k1 , k 2 )G (k1 , k 2 ) = e jθ ( k1 ,k2 ) (3) F (k1 , k 2 )G (k1 , k 2 ) ∧ Phase-Based 2D Inverse of a function shown in the following equation : 1 r (n1 , n2 ) N1 N 2 ∧ ∧ − k1n1 N1 ∑ R(k , k )W 1 2 R (k1 , k 2 ) k1k 2 WN−2k2 n2 (4) (b) (a) Figure 3. (a) PBIM graphs for identical image (b) PBIM graphs for not identical image Figure 2. Stages of the superresolution In this case : • F ( k1 , k 2 ) and G ( k1 , k 2 ) denote Discrete Fourier Transforms (DFT) from spatial domain f ( n1 , n2 ) and g ( n1 , n2 ) • n1 and n2 are elemen index in spatial domain at f (n1 , n2 ) • k1 and k 2 are elemen index in frekuency domain at F (k1 , k 2 ) • k1 = − M 1 ,...,M 1 , k 2 = − M 2 ,...,M 2 • AF (k1 , k 2 ) and AG (k1 , k 2 ) is the 2.2. Sub-Pixel Level Translation amplitude component • e jθ F ( k1 , k2 ) component. e jθ G ( k1 , k 2 ) The results of Phase-Based Functions for the function f (n1 , n2 ) and g (n1 , n2 ) which images are identical, it is obtained height of the dominant graph as shown above. While for the function which images are not identical, it is obtained graph that do not have the dominant height Figure 3 shows a graph of two images which are identical and not identical. The identical image, has a value cross phase spectrum high, while the other one, no value cross phase spectrum high. The coordinates of the cross spectrum of the highest phase, expressed in units of pixels translation between two images. For example, the highest peak position of a graph PBIM located at coordinates (1,2) This indicates, the first image and second image of a global translation in direction as far as 1 unit in x and 2 units in y direction. is the phase Image is processed using a computer is a digital image. During the digitizing process, many of information is lost, one of which is pixels 247 Journal of Theoretical and Applied Information Technology 30th September 2012. Vol. 43 No.2 © 2005 - 2012 JATIT & LLS. All rights reserved. ISSN: 1992-8645 www.jatit.org translation. At continuous images, pixels translation are in the form of real number, but after digitizing, real translation information is lost. Therefore, we need a way to get the actual translation. One method to obtain the actual translation is by fitting of the function PBIM. At phase correlation, sub-pixels translation will be searched by performing iteration around the peak position. Fitting the function can be be used to obtain the actual translation, which is [8][9]: _ r (n1 , n2 ) ≅ α N1 N 2 sin[π (n1 + δ1 )] sin[π (n2 + δ 2 )] π  π  sin  (n1 + δ 1 ) sin  ( n2 + δ 2 )  N N  1   2  (5) In fitting process it is use least square quadratic, in order to obtain the value δ 1 and δ 2 which are translation in the sub pixel level. In this case : • N1 x N2 is dimension of images • n is element in matrix N1 x N2 • δ is a shift in the subpixel level • α≤1 Therefore, these parameters must be known in advance and then made into image density. In addition, the function is created using gaussian applicability function anisotropic. This iteration process is called the Structure Adaptive Normalized convolution. Normalized convolution is a technique to modelling the projection of the local signals into a single set of basis functions. Although there are lots of basis functions that can be used, but the commonly used basis functions is the polynomial where 1=[11…]T basis {1,‫ݔ‬,‫ݕ‬,‫ݔ‬2,‫ݕ‬2,‫ݕݔ‬,...}, T (Nseries), ‫ݔ[=ݔ‬1‫ݔ‬2....‫ ] ܰݔ‬, ‫ݔ‬2=[‫ݔ‬12‫ݔ‬22....‫ܰݔ‬2]T and so forth, which reconstructed from the local coordinates of N samples of input. The use of polynomial basis functions makes Normalized convolution become the same with the expanded local Taylor series. The center of local neighbourhood is in the equation ܵ0= (‫ݔ‬0,0), while the intensity value is in the position of s = (‫ݔ‬+x0,‫ݕ‬+y0) that approximated by an extended polynomial. fˆ ( s, s0 ) = p0 ( s0 ) + p1 ( s0 ) x + p2 ( s0 ) + p3 ( s0 ) x 2 + p4 ( s0 ) xy + p1 ( s0 ) y 2 + ... 3. HIGH RESOLUTION IMAGE RECONSTRUCTION After a series of low-resolution image was registered to obtain the displacement of pixels, then the parameters translational and rotational displacement the images will be used for the reconstruction process. One image in a series of low-resolution image will be used as a reference in the reconstruction. Translational and rotational parameters values pixel displacement is used for projection on a grid of high resolution image. In the next section it will be reviewed the reconstruction algorithms, SANC and POCs algorithms. SANC algorithm is an image interpolation algorithms that work on the scope of Normalized convolution. The next process searches basic functions derived from the value of certainty in these images. After that the values are operated by equation (6). The operation is the Normalized convolution process. (7) where (‫ݔ‬,‫ )ݕ‬is the local coordinates of the sample‫ݏ‬ associated with the center ‫ݏ‬0. (‫ݏ‬0) = [‫݌‬0‫݌‬1‫݌‬2 .....‫]݉݌‬. Where ‫ݏ‬0 is the projection coefficient of the polynomial basis function relationships at ‫ݏ‬0. Adaptive Structures Normalized convolution system uses the information on the structure and distance between the actual image data input to increase the level of the Normalized convolution. The equation (8) and (9) below are used to obtain Gradient the Structure Tensor (GST) in order to build an adaptive kernel in pixels output in the local structure of image. 3.1. Structure-Adaptive Normalized Eonvolution Algorithm (Sanc) ‫)ܤܹܶܤ( = ݌‬−1‫݂ܹܶܤ‬ E-ISSN: 1817-3195  I x2 I x I y  GST = ∇I∇I T =  = λu uu T + λv vvT 2  I x I x I y  φ = arg( u ), A = λu − λv λu + λv (8) (9) Where ∅ is main axis and A is the intensity of the anisotropic. Both of them are calculated from the eigenvector ‫ݑ‬,‫ ݒ‬that correspondd to the eigenvalue λ u ≥ λ v .I x = (6) To create sharper image, the process should be repeated, but with the addition of other parameters, such as estimate local image structure and scale. ∂I ∂x , where I y = ∂I ∂y is the gradient correspondent. Other important characteristics of the data are the local sample density, because it illustrates how much 248 Journal of Theoretical and Applied Information Technology 30th September 2012. Vol. 43 No.2 © 2005 - 2012 JATIT & LLS. All rights reserved. ISSN: 1992-8645 www.jatit.org information that available at grid points near the high-resolution. The adaptive applicability function is an anisotropic Gaussian function which the main axis is rotated to adjust the orientation of the local dominant. α ( s , s exp        0 ρ (( s − s ) =  x cos θ −  σ   −   θ x cos σ v 0 ) + y sin ( s 0 ) θ    2 + y sin ( s 0 ) θ    2 u  −       E-ISSN: 1817-3195 projection operator Pi in each f ( x , y ) then obtained f k +1 = TcmTcm −1.....Tc1 f (12) Where Tc = I + λ ( Pc − I ) i i i projection operator Pci the projecting signal f ( x , y ) to the set of convex the Ci dan λi is the multiplier with a value of 0 < λi < 2. (equation 12). Low-resolution image g ( x , y ) used can be (10) modeled as a high resolution image f ( x , y ) who Where ‫ݏ‬0 = ‫ݔ‬0, 0 is the central of this analysis, ‫ݏ‬−‫ݏ‬0 = ‫ ݔ‬is the local coordinate input samples associated with ‫ݏ‬0, while ߩ is a pillbox function that centered at the origin which restricts the kernel to certain radius. In equation (10), and are the scales of the Anisotropic Gaussian kernel. is the scale that extends along the orientation and greater than or equal to ߪ‫ݑ‬. Then both scales are adjusted to the local scale ߪܿ. α α+A σu = σ c ,σ v = σc α+A α Another algorithm in image reconstruction that quite effective to improve the quality of image with blur and noise is POCs. POCs is not just a fairly simple algorithm, but it also can provide more detailed information of the reconstructed image. This algorithm is the iterative approach to perform the repetitive use of information from a series of low-resolution image and limiting the set of solutions to convex [14,15] If a signal f ( x , y ) and the set of convex C i assumed to be an element in Hilbert and f ∈ C 0 = , i = 1,2..m m IC i noise N ( x , y ) as the following equation: g(x, y) = h( x, y) f ( x + sx , y + sy ) + N (x, y) (13) So that the set of equations is obtained convex (11) 3.2. Projection Onto Convex Sets Algorithm (Pocs) ∈H of degradation or blurring by a point spread the addition of function h ( x , y ) and Ci as follows: Parameters and functions used for highresolution image reconstruction should use enough characteristic of image structure and detail of information, while the shape and size of the local neighborhood can be set adaptively. space, then C i experienced a shift ( s x , s y ) and undergo a process , provided that the slices in i =1 C0 not zero. Given a set of constraints on C and the Ci = { f :| g ( x, y ) − h( x, y) f ( x, y ) ≤ N ( x, y)} (14) Completion of the equation (14) is obtained by iteration of orthogonal projection to a convex set defined by the constraints of low-resolution image noise level, then the projection operator which is obtained substituted into equation (11) to obtain the following equation : f k +1 = f k + λi where g i is g i − hi ' f k ith hi 2 hi (15) 2 element of vector g ( x , y ) and hi ' is a line to iof matrix h ( x , y ) . An initial high resolution image called the Image Super Resolution (SRI) is projected sequentially onto the set of constraints that are built around the components of the observation image g ( x , y ) the so called low-resolution image (LRI). Projections made in the frequency domain. Figure 4 shows an illustration of the POCs in the frequency domain. On the right side of the circuit depicted low resolution image (LRI), which through the process to define the image preprocessing is important and will be used in the reconstruction process, if all the image used then this process can be by passed. 249 Journal of Theoretical and Applied Information Technology 30th September 2012. Vol. 43 No.2 © 2005 - 2012 JATIT & LLS. All rights reserved. ISSN: 1992-8645 www.jatit.org E-ISSN: 1817-3195 The scenarios of testing in this study are as follows : (a) a test image in (figure 5) was assumed to be a high-resolution image; (b) image downsampling was performed to obtain image with low resolution; (c) in addition to lowering the resolution, downsampling also produced a number of image in the same scene; (d) a number of these images were registered using PBIM, Keren and Marcel, then reconstruction of the registration was used to produce a high resolution image; (e) finally, the results of this reconstruction was compared to the test images to obtain the value of PSNR. Table 1 shows the PSNR values of image registration using PBIM collaboration and reconstruction using two reconstruction algorithms, POCs algorithm and SANC algorithm. Figure 4. Illustration of POCs in the frequency domain Table 1. PSNR results, SR with POCs Reconstruction algorithm LRI to be used in the process of reconstruction in the Fourier transform into LRS. On the left is defined initial high-resolution image (SRI) obtained from the LRI which has been scaled or from a simple interpolation methods as nearest, bilinear, or bicubic. SRI in the re sample to adjust to the LRI, in this case when the rotation the LRI experience on SRI is also subject to rotation. SRI then transformed with a Fourier transform image Super Resolution Overlay (SRO).SRO later in the projection in order to set constraints are defined using the LRS. POCs Reconstruction Algorithm 4. RESULT AND DISCUSSION The purpose of this experiment was to get the best performance of collaboration between PBIM, Keren and Marcel registration with SANC and POCs reconstruction algorithm. Registration Num of images PBIM Keren Marcel 4 31.4865 31.4956 30.8905 10 32.25 31.4819 31.4956 20 32.2499 31.8698 30.9888 30 32.2495 31.8697 30.9888 50 32.2486 32.0532 30.9863 100 32.2478 32.0532 30.3825 Avg 32.12205 31.8039 30.9554 There are six experiments results from collaboration of three registration, PBIM, Keren and Marcel registration algorithm with variant LR images. Table 1 also shows the highest average of PSNR that achieved in collaboration between PBIM registration with POCs algorithm and has PSNR average value of 32.12205. Collaboration between Keren registration and POCs algorithm reconstruction has an average PSNR value of 31.8039. The Marcel registration has an average PSNR value of 30.9554 while Keren and Marcel registration has lower PSNR value than the PBIM registration. It shows that the registration PBIM is better than Keren and Marcel registration. Figure 5. Test images 250 Journal of Theoretical and Applied Information Technology 30th September 2012. Vol. 43 No.2 © 2005 - 2012 JATIT & LLS. All rights reserved. ISSN: 1992-8645 www.jatit.org The results of this test are presented in Table 2. This tabel shows a comparison between PBIM, Keren and Marcel registration, which collaborated with the SANC reconstruction algorithm. The results show that PBIM registration with fitting function has a higher PSNR values compared with Keren and Marcel registration. 33 32.5 32 31.5 PSNR E-ISSN: 1817-3195 31 Table 2. PSNR results, SR with SANC Reconstruction algorithm 30.5 30 SANC Reconstruction Algorithm 29.5 4 10 20 30 Num of images Registration Num of images 29 50 Figure 6. PSNR graph for POCs reconstruction Algorithm Figure 6 presents a graph of the relationship between PSNR value and the number of reference images used for reconstruction. Image used in this experiment is an aircraft image (figure 7a). While Figure 7b shows the SR results using PBIM Registration with POCs reconstruction algorithm. PBIM Keren Marcel 4 31.597 31.4553 31.0116 10 32.0968 31.4032 30.1018 20 32.0838 31.2691 29.9189 30 32.2367 31.3164 29.9964 50 32.2098 31.3197 29.9068 100 32.2154 31.3037 29.8825 Avg 32.07325 31.3445 30.1363 Figure 8 shows the relationship between PSNR value and various numbers of reference images, and collaboration between PBIM and various of registration. . 33 32.5 PSNR 32 31.5 31 30.5 30 (a) LR images 29.5 29 4 PBIM-SANC 10 20 30 Num of images Keren-SANC 50 100 Marcel-SANC Figure 8. PSNR graph for SANC reconstruction Algorithm (b) HR, output of SR Figure 9 shows the SR results for real image. Figure 9(a) is an image was extracted from video, taken with DCR-HC52E, 30 fps Sony handycame. Figure 7. The result of SR 251 Journal of Theoretical and Applied Information Technology 30th September 2012. Vol. 43 No.2 © 2005 - 2012 JATIT & LLS. All rights reserved. ISSN: 1992-8645 www.jatit.org E-ISSN: 1817-3195 REFERENCES : (a) LR image (b) HR, output of SR Figure 9. The result SR from real images While Figure 9(b) show our SR result with PBIM registration. 5. 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