INFRARED TARGET EXTRACTION ALGORITHM BY USING PARTICLE SWARM OPTIM IZATION PARTICLE FILTER
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1 J. Infrared M illim. W aves Vol. 29, o. 1 February, 2010 : (2010) , 2 (1., ; 2., ) : ( PSOPF),.,,,,.,.,. : ;; ; : TP391. 4: A IFRARD TART XTRACTIO ALORITHM BY USI PARTICL SWARM OPTIM IZATIO PARTICL FILTR ZHOU Yue 1, MAO Xiao2an 2 (1. Institute of Pattern Recognition and Image Processing, Shanghai J iaotong University, Shanghai200240, China; 2. Control ngineering Institute of SAST, Shanghai200233, China) Abstract: A novel infrared target extraction algorithm based on particle swarm op tim ization particle filter ( PSOPF) was p roposed. The p roblem of infrared target extraction was analyzed and solved in the view of state estimation. In the frame2 wor of particle filter, the threshold state space on the gray2variance weighted information entropy and the gray value of each p ixel was established. Particle swarm op tim ization was introduced to construct the state transition model. The observation model based on extraction results evaluation function was constructed, which integrated gray, entropy, gradient and spatial distribution of p ixels. Finally, the weighted average of all the particles was used as target extraction threshold. The experi2 ment results p rove that the p roposed algorithm is effective and robust. Key words: particle filter; particle swarm op tim ization; target extraction; gray2variance weighted information entropy,,., [ 1, 2 ] [ 3 ] [ 4 ]. (),, [ 2 ] [ 5 ]. O tsu, [ 1, 2 ],,, [ 6, 7 ]., ( ),., [ 8, 9 ]. [ 6 ] Kennedyberhart 1995.,, : , : Rece ived da te: , rev ised da te: : ( ) ; : ( ),,,,, 2Mail: zhouyue@ sjtu. edu. cn.
2 64 29,, [ 7 ]. :,, ;,, ;,, ;,,,. 1, R T.,, R T,. S bg, S obj,s bg S obj =, S bg S obj = R T. S obj. 1. 1, R T 2 S U : = 1 K K i, (1), KR T ; U = 1 U U s i, (2), U S U, s i S U i ; i = i H i, (3), i i, H i i [ 10 ]. = 1, T = 1, T = 2 2 U S U,S U, T T,. T T, = 1, 0 < 1 < 2 { i }, 2,, K, 0 < 2 { s i }, 2, U <, U, [ 9 ],.,, 0, 0,, 2,, U { s i } U, 2,, K { i },, w 0 = 1., ( ) L ( ) : ( ) L = arg{w ( l),, w,, w ( ) }, i = 1, 2, (4) ( ) = arg{w ( l),, w,, w ( ), w ( - 1) }, L = 1, 2, (5), w i, w ( - 1) - 1 ( - 1). 1,. 1 = 0 + U 1 = 1 = ( ( - 1) - - 1) U 1 + ( ( - 1) L ) - - 1) U 2 2,, (6), U 1, U 1, U 2, i = 1, 2,,. ( 7) , ,,,.
3 1 : 65 = 1 s j, (7) j =1, i = [ 1,, 2, ] T S..,,. : ( d i, j ) = d2 1 2 e- 22, (8) R T ( i, j) ( d i, j ), d R T ; R T H R T W R T, = 10 H R T W R T. i = [ 1,, 2, ] T S :, = 1 ( d j ) j, (9) j =1, d j S j R T, j j. { }, 2,,. Sobel,. : rad = 1 g 2 1, j + g 2 2, j, (10) j =1, S, g 1, j g 2, j S. { rad j }, 2,,. i = [ 1,, 2, ] T S, O,S O. Con = 1 P j =1 j, - O. (11) :S ,,.,,. { ( l), (2),, ( ) }, { S (1), S (2),, S ( ), }, = [ ( 1), (2),, ( ), ] T, m v, : = - m v. (12) ( x) = 1 x2 2 e- 2 =( ),., { Con { }, 2,,., : V = 4, exp ( 1, = 2, = 3, = 4, =, rad Con 1,, 2,, 3,, }, 2,,, 1, 2, 3, ), (13) 4,. = {, w } :,w : = V w V. (14) = gw. (15),. 1 ( a1) ( a4)( b1) ( b4),. 3,,., ( a1) ( a4 )( a1 ), ( b1 ) ( b4)( b1). ( 13),1. = 15,1.
4 ( = 15) Fig. 1The extracting results with different thresholds ( number of particles = 15) 1 Table 1The results of the eva lua tion function V ( ) () () ( ) rad ( ) () a a a a b b b b i = 1:, = [, 1,, 2 ] T, (15) w., (5) (6) 4. (16), +1 -,, ; [ 9 ], :. : , = 011;,,, = 011,. 1.., 0 < 1 <, 2,, K { i }, 0 < 2 <, 2,, U { s i } U,, 0 = { 0, w 0 }, 2,,, w 0 = 1, = (7) = {, w } :. Pentium 2. 40Hz PC VC , 2 ( a) ( e). 2( a) ( b)( c),,2d2 ( c), 2D2 ( a) ( b). ( d) ( e), 2D2 2D2,,.,2D2O tsu,, , [ 2 ] PSO, 15, 11, 165.,15, 3, 45
5 1 : 67 23, 2D2 2D2 Fig. 2The comparison of 3 target extraction algorithm s, the original image, our algorithm, 2D2O tsu, 2D2imum entropy method from left to right,. 3,.,,, 2D2O tsu,.,
6 68 29,,.. RFRCS [ 1 ] ZHA Tian2Xu, ZHAO uang2zhou, WA Fei, et al. Fast recursive algorithm for infrared ship image segmentaion [ J ]. J. Infrared M illim. W aves(,,,.. ), 2006, 25 (4) : [ 2 ]DU Feng, SH IW en2ka, D Yong, et al. Fast infra2 red image segmentation method [ J ]. J. Infrared M illim. W aves (,,,.. ), 2005, 24 (3) : [ 3 ] SU W ei, X IA L iang2zheng. Infrared target segmentation algorithm based on morphological method [ J ]. J. Infrared M illim. W aves (,.. ), 2004, 23 ( 3 ) : [ 4 ] TAO W en2bing, J I Hai. Ship infrared object segmentation based on mean shift filtering and graph special clustering [ J ]. J. Infrared M illim. W aves(,.. ), 2007, 26 (1) : [ 5 ]R J i2jun, H M ing2yi. Level set method of image seg2 mentation based on imp roved C2V model of 32D histogram ( 9) Radiation effects on photonic imagers2a historical perspec2 tive[ J ]. I Trans. ucl. Sci. 2003, 50: [ 2 ]HU Xin2W en, ZHAO Jun, LU Hui2Q ing, et al. amma ir2 radiation on room temperature short2wavelength HgCdTe photovoltaic device studied by adm ittance spectroscopy[ J ]. A cta Physica S inica (,,,. HgCdTe. ), 1999, 48 (6) : [ 3 ]L IAO Yi, WA J ian2xin, ZHA Q in2yao. amma ra2 diation effects on MW IR HgCdTe FPA device [ J ]. Chinese Journal of Q uantum lectronics (,,.. ), 2007, 24 (1) : [ 4 ] opal V, up ta S, Bhan R K, et al. Modeling of dar characteristics of mercury cadm ium telluride n + p junctions [ J ]. Infrared Physics & Technology, 2003, 44: [ 5 ]guyen T H, Musca C A, Dell J M, et al. The effects of vacuum baing on the IV characteristics of LW IR HgCdTe photodiodes[ J ]. P roceedings of SPI, 2004, 5274: [ 6 ] SU Tao, CH Xin2uo, HU Xiao2 ing, et al. Low2fre2 quency noise of Hg 12x Cd x Te long2wavelength photovoltaic detector[ J ]. J. Infrared M illim. W aves (,,,. Hg 1 - x Cd x Te. ). 2005, 24 (4) : [ 7 ] ZHA Xin2Chang, ZHA Q in2yao, XU Zhen, et al. A study of interface electrical characteristics for CdTe / ZnS passivation film s[ J ]. J. Infrared M illim. W aves (, [ J ]. J. Infrared M illim. W aves (,. C2V. ), 2008, 27 (1) : [ 6 ] Kennedy J, berhart R. Particle swarm op tim ization [ J ]. eural etw ors, 1995, Proceedings., I International Conference on Volume4, 27ov. - 1Dec Page ( s) : [ 7 ] FA Zheng, TO uo2feng, XU Xin2He. Particle swarm op tim ized particle filter[ J ]. J. Control and D ecision (,,.. ), 2007, 22 (3) : [ 8 ] Isard M., B lae A. CODSATIOConditional density p ropagation for visual tracing[ J ]. International Journal of Com puter V ision, 1998, 29 (1) : 528. [ 9 ]Cheng J ian. Research on V isual Tracing A lgorithm s Based on Particle Filtering and Their App lications in Infrared Imaging uidance [ D ]. Shanghai: Shanghai J iaotong University, 2006 (.. : ), 2006: 3132 [ 10 ]Lei Yang, J ie Yang, ingsong Peng, et al. W eighted In2 formation ntropy: A Method for stimating the Comp lex Degree of Infrared ImagesBacgrounds[ C ]. Internation2 al Conference of Im age A nalysis and Recognition 2005 ( IC IAR 2005 ). Lecture otes in Computer Science. 3656, ,,. CdTe /ZnS. ). 1996, 15 (6) : [ 8 ]W illardson R K, Beer A C. Sem iconductors and Sem im et2 als. V ol. 18 [M ]. ew Yor: Academ ic Press, 1981, 201. [ 9 ]em irovsy Y, Uniovsy A. Tunneling and 1 /f noise cur2 rents in HgCdTe photodiodes[ J ]. J. V ac. Sci. Technol. B. 1992, 10 (40) : [ 10 ]RaisM H, Musca C A, Antoszewsi J, et al. Characteri2 sation of dar current in novel Hg 1 - x Cd x Te m id2wavelength infrared photovoltaic detectors based on n2on2p junctions formed by p lasma2induced type conversion [ J ]. J. C rystal row th, 2000, 214 /215: [ 11 ]QUA Z J, L I Z F, HU W D, et al. Parameter determ ina2 tion from resistance2voltage curve for long2wavelength HgCdTe photodiode[ J ]. Journal of A pplied Physics. 2006, 100: [ 12 ]Q IAO Hui, ZHOU W en2hong, Y Zhen2Hua, et al. study on variable2area hydrogenation of hgcdtephotovoltaic de2 tectors[ J ]. J. Infrared M illim. W aves (,,,.. ). 2008, 27 (6) : [ 13 ] CHU Jun2Hao. arrow bandgap sem iconductor physics [M ]. Beijing: Science Press (.. :) 2005, 458. [ 14 ]CAO J ian2zhong. Radiation effects of sem iconductorm ateri2 als[m ]. Beijing: Science Press (.. :), 1993, 66.
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