ITERATIVE DECODING OF TURBO CODES

Size: px
Start display at page:

Download "ITERATIVE DECODING OF TURBO CODES"

Transcription

1 Journal of Advanced College of Engineering and Manageent, Vol.3, 07 ITERATIVE DECODIG OF TURBO CODES Dhanehwar Sah Advanced College of Engineering and Manageent, T.U. Eail Addre: Abtract Thi paper preent a Thei which conit of a tudy of turbo code a an error-control Code and the oftware ipleentation of two different decoder, naely the Maxiu a Poteriori (MAP), and oft- Output Viterbi Algorith (SOVA) decoder. Turbo code were introduced in 993 by berrouet at [] and are perhap the ot exciting and potentially iportant developent in coding theory in recent year. They achieve near- Shannon-Liit error correction perforance with relatively iple coponent code and large interleaver. They can be contructed by concatenating at leat two coponent code in a parallel fahion, eparated by an interleaver. The convolutional code can achieve very good reult. In order of a concatenated chee uch a a turbo code to wor properly, the decoding algorith ut affect an exchange of oft inforation between coponent decoder. The concept behind turbo decoding i to pa oft inforation fro the output of one decoder to the input of the ucceeding one, and to iterate thi proce everal tie to produce better deciion. Turbo code are till in the proce of tandardization but future application will include obile counication yte, deep pace counication, teleetry and ultiedia. Finally, we will copare thee two algorith which have le coplexity and which can produce better perforance. Keyword: SOVA, MAP, SISO, Turbo Code, RSC, Channel Model, SR, BER, LLR, VA. Introduction One of the ai of thi paper will be to how that copriing and analyi for different decoding algorith of turbo code. There are variou iterative decoding technique. SISO: Soft inforation, or reliability, i crucial inforation type when turbo-lie (iterative) proceing of data i conidered. With the advent of turbo code in the area of inforation theory, a lot of attention i given to algorith that can provide uch oft reliability value while decoding the original inforation. There are two nown oft-input oft-output. The thei i propoed to wor on thee two SISO decoding Method: Maxiu a Poteriori (MAP) decoding algorith and SOVA (Soft Output Viterbi Algorith). Thi algorith i ued to iniize the probability of word or equence error.it wor by rejecting the leat liely path through the trelli at each node, and eeping the ot liely one. The reoval of unliely path leave u, uually, with a ingle ource path further bac in the trelli. Thi path election repreent a hard deciion on the tranitted equence. The Viterbi decoder etiate a axiu lielihood equence.. Turbo Code Turbo code were dicovered in 993 [] before that, Shannon liit on code perforance could only be approached with very long code word length. There wa the proble of decoder coplexity a well [9]. But we hall analyze in thi chapter how decoder coplexity can be reduced while ipleenting turbo code.. Encoder A parallel concatenated convolutional code i ued for encoding turbo code. In the Fig [] d i = (d, d, d 3..d ) repreent the binary input data equence which i paed into the input of 5 jace, Vol.3, 07 Iterative Decoding of Turbo Code

2 convolutional encoder [4][3] EC, a denoted in the original paper. A a reult, a coded bit trea P xk i generated which i then interleaved, often in a peudo-rando pattern. The interleaved data equence i paed to a econd convolutional encoder EC and another coded bit trea x i produced. Both of the code bit trea a yteatic code bit 5 x and parity bit x and x are ultiplexed (and poibly punctured) to for P K p x P K P K d K p x x Peudo- Rando Interleaver EC p x Channel EC p x Fig Turbo Encoder. Recurive Syteatic Convolutional (RSC) code The convolution (RSC) coder EC and EC ued turbo encoder are recurive yteatic convolutional (RSC) code. RSC code are the convolutional code that ue feedbac and the uncoded data bit are alo preent in the tranitted code bit equence. Fig how a RSC encoder. The hown RSC encoder i of rate /, with contraint length = 3, and a generator polynoial G = {g, g} = {7, 5}, where g i the feedbac connectivity and g i the output connectivity, in octal notation. An x = x x,..., x and parity RSC coponent encoder ha two output equence: data: equence (, ) p p p p equence x = ( x x,..., x ). d K, x + a a - a - + p x Fig Recurive Syteatic Convolution Code The linear nature of turbo code (at leat, thoe uing BPSK/QPSK odulation) ean that the iniu Haing ditance of the code can be deterined by coparing each Poible code wordwith the all zeroe codeword.thi proce iplifie analyi of the code oewhat and the iniu haing ditance i then equal to the iniu codeweight (nuber of ) which occur 6 jace, Vol.3, 07 Iterative Decoding of Turbo Code

3 in any codeword.. Thi i the relationhip between the codeweight and the nuber of codeword with that codeweight. An SC code, however, will return to the all zeroe tate after - input zeroe, where K i the contraint length of the encoder. The infinite ipule repone property of RSC code i copleented in turbo code by the interleaver between coponent encoder. The reult i a copoite codeword which will often have a high codeweight.. The peudo-rando nature of ot turbo code interleaver tend to reult in a apping uch that a few cobination of input bit poition which caue low codeweight equence in one RSC coponent code are peruted into cobination of poition which generate low codeweight equence in the econd RSC code. The reult in uch a cae are a low copoite codeweight. uch peudo-rando apping often lead to turbo code having a low iniu codeweight copared to ay, SC-baed convolutional code, reulting in a ared error floor at high SR.. The ditance pectru of the code a a whole becoe ignificant in deterining BER perforance, and that the cobination of RSC code and peudorando interleaving produce codeword with higher code weight ot of the tie. The low ultiplicity of low codeweiught equence aociate with turbo code oetie referred to a pectral thinning, lead to their good BER perforance at low SR..3 Interleaver An interleaver doe the wor of re-arranging a equence of ybol. One ue of interleaver in counication i that of the ybol interleaver which i ued after error control coding and ignal apping to enure that fading burt affecting bloc of ybol tranitted over the channel are broen up at the receiver by a de-interleaver, prior to decoding. Mot error control code wor uch better when error in the received equence are pread far apart. Another ue i to place an interleaver between coponent code in a erially concatenated code chee for exaple, between a Reed Soloon outer code and a convolutional inner code. In both cae, the interleaver i typically ipleented a a bloc interleaver. The original data equence i repreented by the equence of white quare, and the interleaved data equence i repreented by the grey quare. Berrou and Glavieux original paper [] featured reult uing a 56*56 interleaver. Turbo code BER perforance iprove with interleaver length-the o called interleaver gain- but the loading and unloading of the interleaver add a coniderable delay to the decoding proce. Thi would ae a 56*56 interleaver unuitable for ay real tie peech application which are delay enitive..6 Terination Convolutional coding i a continuou proce and code word do not have a fixed bloc length. The proce can pan the whole eage rather than a all group of bit. But the turbo code do have the fixed bloc length which i a deterined by the length of the interleaver. Uual procedure i to append tail bit to each bloc of data bit entering one or other of the coponent encoder, to return it to the all zero tate at the end of the trelli. Thi proce i called terination 3. Turbo Decoding The turbo decoder conit of two coponent decoder: DEC to decode the equence fro EC and DEC decode the equence fro EC. Both DEC are Maxiu a poteriori (MAP) decoder. DEC tae the received equence of yteatic value y and the received equence of parity value belonging to the firt encoder EC. The output of the decoder DEC i equence of oft etiate EXT of the tranitted data bit d. The EXT i called the extrinic data, in that it doe not contain any inforation which wa given to DEC to DEC. Thi inforation i interleaved, and then paed to the econd decoder DEC. The encoder i identical to the ued in the encoder. DEC tae a it y 7 jace, Vol.3, 07 Iterative Decoding of Turbo Code

4 input the interleaved yteatic received value y and the equence of received parity value fro the econd encoder EC along with the interleaved fro of the extrinic inforation EXT, provided by the firt decoder. The econd decoder DEC produce a it output a et of value which when de-interleaved uing the invere for of interleaver, contitute oft etiate EXT of the tranitted data equence d. Thi extrinic data, fored without the aid of parity bit fro the firt code, i feedbac to DEC. Thi procedure i repeated in an iterative anner. The iterative decoding proce add greatly to the BER perforance of turbo code for exaple, Berrou and Glavieux Eb achieved BER = 0 5 at within 0.7 db of the Shannon liit, uing a rate / turbo code and 8 o decoding iteration. However, after everal iteration, the two decoder etiate of d will tend to coverage. At thi point, DEC output a value Λ( d ) a log lielihood repreentation of the etiate of d.thi log- lielihood value tae into account the probability of a tranitted 0 or baed on the yteatic inforation and parity inforation fro both coponent code. More negative value of Λ( d ) repreent a trong lielihood that the tranitted bit wa a 0 and ore poitive value repreent a trong lielihood that it wa tranitted bit. Λ( d ) i de- interleaved o that it equence coincide with that of the yteatic and firt parity trea. Then a iple threhold operation i perfored on the reult, to produce hard deciion etiate, d for the tranitted bit. The decoding etiate EXT and EXT, do not necearily converge to a correct bit deciion. If a et of corrupted code bit for a pair of error equence that neither of the decoder i able to correct, then EXT and EXT ay either diverge, or converge to incorrect oft value. Deinterleaver y EXT EXT Interleaver DEC DEC EXT y p y interleaver Λ( d ) Deux y p y Deinterleaver =, Fig 3 Turbo Decoder Structure 8 jace, Vol.3, 07 Iterative Decoding of Turbo Code

5 3. The MAP Algorith The decoding algorith ipleented in DEC and DEC for iterative decoding need to be analyzed. The firt one under dicuion i the Maxiu A poteriori (MAP) algorith preented in Berrouet. al original paper []. We decribe here a derivation of the MAP decoding algorith for yteatic convolutional auing an AWG channel odel, a preented by pietrobo [6]. 4. Channel odel In additive white Gauian noie channel, the received ignal i the u of the tranitted (attenuated in oe way) and noie with a Gauian probability denity function (pdf) given by: p (n) = exp n (3.6) The effect of AWG i to hinder a detector in the etiate of the tranitted ignal baed on a poibly very wea received ignal. Becaue AWG affect all electronic circuitry, it alot alway added to a iulation channel odel. 4. Perforance of Turbo Code for Log-MAP A iulation progra ha been written and it give the perforance for and length data. However, it tae uch tie depending on data length, punctured or unpunctured pattern, the Eb/0 ratio provided and the channel odel ued.an analyi wa done on an AWG channel for rate /, length 04-bit and log MAP Turbo decoder. We oberve the gain achieved by the turbo code relative to convolutional code of relative coplexity. We can clearly ee the iterative power of turbo code. Fig 4 Perforance of 400 bit, rate /, log-map Turbo Code veru ratefour State Convolutional Code over AWG 9 jace, Vol.3, 07 Iterative Decoding of Turbo Code

6 Fig 5 Perforance of 04 bit, rate / log-map Turbo Code veru rate / fourtate convolutional Code over AWG. Log-Map over AWG Fig 6 Perforance of 04 bit, rate /, log-map Turbo Code veru rate/fourtate convolutional Code over AWG. 4. Soft Output Virtebri Algorith (SOVA) Thi algorith i ued to iniize the probability or word or equence error. It will wor by rejecting the leat liely path through the trelli at each node, and eeping the ot liely one. The reoval of unliely path leave u, uually, with a ingle ource path further bac in the trelli. Thi path election repreent a hard deciion on the tranitted equence. The Viterbi decoder etiate a axiu lielihood equence. 0 jace, Vol.3, 07 Iterative Decoding of Turbo Code

7 It i decribed here a derivation of MAP decoding algorith for yteatic convolutional code auing an AWG channel odel, a preented by pietrobon [6]. We tart with the ratio of the APP, nown a the lielihood Ratio Λ( ), or it logarith, called the LLR, a hown below. Where Λ ( d ) = λ λ Ld ( ) = log λ i, binary equence i, 0, λ λ i, 0, (4.) (4.) the joint probability that data = and tate = conditioned on the received R oberved fro tie = through oe tie, i decribed a λ = pd ( = is, = R ) i, (4.3) R Repreent a corrupted code bit equence after it ha been tranitted through the channel, deodulated, and preented to the decode in oft deciion for. In effect, the MAP algorith require that the output equence fro the deodulator be preented to the decoder a a bloc of bit at a tie. Let R be written a follow, {,, + } R = R R R To facilitate the ue of Baye theore, Equation (4.) i partitioned uing the letter A, B, C, D and Equation (4.3). Equation (4.) can be written in thi for: (4.4) λ = pd ( = is, = R, R, R ) i, (4.5) A = p( d = i, S = ) B = R C = R and D = R + Fro Baye theore p ( A, B, C, D ) p ( B A, C, D ) P ( A, C, D ) p ( A B, C, D ) = = p ( B, C, D ) p ( B, C, D ) P ( B A, C, D ) P ( D A, C ) P ( A, C ) = P ( B, C, D ) Hence, application of thi rule to Equation (4.5) yield (4.6) y = p( R d = i, S =, R ) p( R d = i, S =, R ) i, + x pd ( = is, = R, ) pr ( ) (4.7) jace, Vol.3, 07 Iterative Decoding of Turbo Code

8 Where { R R } RK =, K + Equation (4.7) can be expreed in a way that give greater eaning to the i, probability ter contributing to λ. The three nuerator factor on the right ide of Equation (4.7) will be defined and developed a the forward tate etric, the revere tate etric, and the branch etric. 4.3 State etric and the Branch Metric We define the firt nuerator factor on the right ide of Equation (4.7) a the forward tate etric at tie K and tate, and denote it a a Thu for i =,0. =, =, = = (4.8) R otice that d = i and are deignated a irrelevant, ince the auption the S = iplie that event before tie are not influenced by obervation after tie K. In other word, the pat i not P R i independent of the fact that d = i and equence R. affected by the future, hence ( ) However, ince the encoder ha eory, the encoder tate S = i baed on the pair, o thi ter i relevant and ut be left in the expreion. The for of Equation (4.8) i intuitively atifying, ince it preent the forward tate etric a at tie a being a probability of the pat equence; that i, dependent only on the current tate induced by thi equence, and nothing ore. Thi hould be failiar fro the econd nuerator factor on the right ide of Equation (4.7) repreent a revere tate etric, β at tie and tate, decribed below =, =, =PR (,) S = (i, ) β (4.9) Where ( i, ) i the next tate, given an input I and tate, and β ( i, ) + i the invere tate etric at tie + and tate ( i, ). The for of Equation (4.9) i intuitively atifying ince it preent the revere tate etric, ( i, ) β + at future tie +, a being a probability of the future equence, which depend on the tate (at future tie ). Thi hould be failiar becaue it create the baic definition of a finite-tate achine [7]. We define the third nuerator factor on the right ide of Equation (4.7) i, a the branch etric at tie and tate. denotedδ Thu we write ( =, =, ), (4.0) Subtituting Equation (4.8) through (4.0) into Equation (4.7) yield the following ore copact expreion for the joint probability: i, (, i) i, aδ βl+ λ = pr ( ) Equation (4.) can be ued to expre Equation (4.) and (4.) a follow: Λ d = a a, (, ) δ β+ 0, (0, ) δ β+ (4.) (4.) jace, Vol.3, 07 Iterative Decoding of Turbo Code

9 , (, ) aδ β + = log 0, (, ) aδ β + L d (4.3) Where Λ i the lielihood ratio of the th data bit and L, the logarith of Λ,i the LLR of the th data bit, where the logarith i generally taen to the bae e. 4.4 Calculating the Forward State Metric Starting fro Equation (4.8), a can be expreed a the uation of all poible tranition probabilitie fro tie -, a follow = ( =, = ', = ) j= 0 a p d j S R S R a{ R R } We can rewrite,, and fro Baye theore, (4.4) = = = = j= 0 a p( R S, d j, S ', R ) pd ( = js, = ', R S = ) x j= 0 ( ) = p ( R S = b( j, ) p( d = j, S = b( j, ), R ) (4.5a) (4.5b) Where b(j,) i the tate going bacward in tie fro tate, via the previou branch correponding to input j. Equation (4.5b) can replace Equation (4.5a) ince nowledge about the tate and the input j, at tie -, copletely, define the path reulting in 4. State S =. Uing Equation (4.8) and Equation (4.0) to iplify the notation of Equation (4.5) yield the following: (,) =,(,) (4.6) Equation (4.6) indicate that a new forward tate etric at tie and tate i obtained by uing two weighted tate etric fro tie -. The weighting conit of the branch etric aociated with the tranition correponding to data bit 0 and. Figure 3. illutrate the ue of two b( j, ) different type of notation for the paraeter alpha. We ue a for the forward tate etric at tie -, when there two poible underlying tate (depending upon whether j=0 or ). And we ue a for the forward tate etric at tie, when the two poible tranition fro the previou tie terinate on the ae tate tie. 3 jace, Vol.3, 07 Iterative Decoding of Turbo Code

10 b (0, a ) J=0 0, b(0, ) δ K a β J=0 0, δ (0, ) a + J= b(, ) a J=, b(, ) δ, δ (, ) β + K- K K K+ (a) Forward tate etric (b) Revere tate etric a = a δ + a b(0, ) 0, b(0, ) b(, ), b(, ) δ β β δ β δ (0, ) 0, (, ), = Where b (j,) i the tate going bacward in where ( i, ) i the next tate going an tie correponding to an input j. input j and tate. 4.5 Branch Metric: δ ( xu yv ) = π exp + i, i i i, Graphical repreentation for calculating a and β []. 4.6 Calculating the Revere State Metric Starting fro Equation (4.9) where = R S = (, i ), (, i) β β + = pr ( S = ) = pr (, R S = ) we how β a follow: (4.7) We can expre β a the uation of all poible tranition probabilitie to tie +, a follow: β + + ' j= 0 Uing Baye theore, = pd ( = js, = R ',, R S = ) (4.8) β ' j= 0 = p( R S =, d = j, S = ', R ) x p( d = j, S = ', R S = ) (4.9) S = and d =j in the firt ter on the right ide of Equation (4.9) copletely define the path reulting in = ( j, ) S K + ) the next tate given an input j and tate. thu, thee condition allow replacing S + = ' with S = in the econd ter of Equation (4.9), yield the following: j, ( j, ) = pr ( S ) ( jpd, ) ( js, R, ) + + = = = = + j= 0 j= 0 β δ β (4.0) 4 jace, Vol.3, 07 Iterative Decoding of Turbo Code

11 Equation (4.0) indicate that a new revere tate etric at tie and tate i obtained by uing two weighted tate etric fro tie +The weighting conit of the branch etric aociated with the tranition correponding to data bit 0 and Figure 3..b illutrate the ue of two different type of notation for the paraeter beta. We ue ( i, β ) + for the revere tate etric at tie + when there are two poible underlying tate (depending on whether j=0 or ). And we ue β for the revere tate etric at tie, where the two poible tranition arriving at tie + te fro the ae tate at tie. Fig 3 repreent a graphical illutration for calculating the forward and revere tate etric. Ipleenting the MAP decoding algorith ha oe iilaritie to ipleenting the Viterbi decoding algorith [3]. In the Viterbi algorith, we add branch etric to tate etric. Then we copare and elect the iniu ditance (axiu lielihood) in order to for the next tate etric. The proce i called add-copare-elect (ACS). In the MAP algorith, we ultiply (add, in the logarithic doain) tate etric by branch etric. Then, intead of coparing the, we u the to for the next forward (or revere) tate etric, a een in figure. The difference hould ae intuitive ene. With the Viterbi algorith, the ot liely equence i being the bet path. With the MAP algorith, oft nuber (lielihood or Log-lielihood) i being ought; hence the proce ue all the etric fro all the poible tranition within a tie interval, in order to coe up with the bet overall tatitic regarding the data bit aociated with that tie interval. 4.7 Calculating the Branch Metric We tart with Equation (4.0), which i rewritten below: δ = pd ( = is, = R, ) = pr ( d = is, = ps ) ( = d = i) pd ( = i) i, (4.) Where R = x, y, x i the received data bit, and y i the correponding noiy received parity bit. Since the noie affecting the data and the parity are independent, the current tate i independent of the current input, and can therefore be any one of the 0 tate, where V i the nuber of eory eleent in the convolution code yte. That i, the contraint length,, of the code i equal to V+. Hence, ps ( = d = i) = v and i δ = p( x d = i, S = ) p( y d = i, S = ) π v (4.) i Where π i defined a p(d =i), the a priori probability of d. The probability p(x =x ) of a rando variable. X taing on the value x i related to the probability denity function (pdf) p x,(x ) a follow [7]. P(X =x )=px,(x )d (4.3) For notational convenience, the rando variablex, which tae on value x, i often tered the rando variable x,which repreent the eaning of X and Y in Equation (4.). Thu, for an AWG channel where the noie ha zero ean and variance, we ue Equation (4.3) in order to replace the probability ter in Equation(4.) with their pdf equivalent, and we write σ 5 jace, Vol.3, 07 Iterative Decoding of Turbo Code

12 δ i i i, i, π x u y v = exp dx exp 0 dy πσ σ πσ (4.4) Where u and v repreent the tranitted data bit and parity bit, repectively (in bipolar for), dx and dy are the differential of x, y and get aborbed into the contant A below. ote that the i i paraeter u repreent data that ha no dependence on the tate. However, the paraeter v, repreent data, which doe depend on the tate, ince the code ha eory. i, i i i, δ = Aπexp ( xu + yv ) σ (4.5) If we ubtitute Equation (4.4) into Equation (), we obtain, yv a exp β x σ Λ ( d ) = π exp 0, σ yv a exp β σ x πexp σ and π e (, ) + (0, ) + (4.6a) (4.6b) (4.6c) L d = L( d) + Lc( x) + Le d 0 Where, π = π / π i the input priori probability ratio (prior lielihood) and π e i the output e extrinic lielihood each at tie. In equation (4.6b), one can thin of π a a correction ter (due to the coding) that change the input prior nowledge about a data bit. In a turbo code, uch correction ter are paed fro one decoder to the next, in order to iprove the lielihood ratio for each data bit, and thu iniize the probability of decoding error. Thu the decoding proce entail the ue of e Equation (4.6b) to Copute Λ for everal iteration. The extrinic lielihood π, reulting fro a particular iteration replace the a priori lielihood ratio π + for the next iteration. Taing the logarith of ( ) in Equation (4.6b) yield Equation (4.6c) which how that the final oft nuber ( )i ade up of three LLR ter: the priori LLR, the channel eaureent LLR, and the extrinic LLR [7]. The MAP algorith can be ipleented in ter of lielihood ratio ( ) a hown in Equation (4.6a) or (4.6b). However, ipleentation uing lielihood ratio i very coplex becaue of the ultiplication operation that are required. By operating the MAP algorith in the logarithic doain [6, 8] a decribed by the LLR in Equation (4.6b) or (4.6c), the coplexity can b greatly reduced by eliinating the ultiplication operation. 4.8 Perforance of Turbo Code for SOVA A iulation progra ha been written and it give the perforance for any length data. However, it tae uch tie depending on data length, punctured or unpunctured pattern, The E b / 0 ratio provided and the channel odel ued. At firt, analyi wa done on an AWG channel for rate / length 400-bit and SOVA turbo decoder. We oberve the gain achieved by the turbo code relative to 6 jace, Vol.3, 07 Iterative Decoding of Turbo Code

13 convolutional code of relatively coplexity. We can clearly ee the iterative power of turbo code figure. Fig 7 Perforance by Siulation of Length 400 bit rate /, and GeneratorPolynoial G = {7,5},Turbo code over AWG Channel. Fig 8 Perforance by iulation oflength 04, Rate / and GeneratorPolynoial G = {7,5}, Turbo Code over AWG Channel. Fig 9 Perforance by Siulation of Length 04, Rate /3 and GeneratorPolynoial G = {7,5} Turbo Code over AWG Channel. 7 jace, Vol.3, 07 Iterative Decoding of Turbo Code

14 4.9 Coparion between the MAP and SOVA The MAP algorith i unlie the Viterbi algorith (VA), where the APP for each data bit i not available. Intead, the VA find the ot liely equence to have tranitted. However, there are iilaritie in the ipleentation of the two algorith. When the decoder bit error probability, PB, i all, there i very little perforance difference between the MAP and Viterbi algorith. However, at low value of bit-energy to noie power pectral denity, Eb/o and high value of PB, the MAP algorith can outperfor decoding with a oft-output Viterbi algorith called SOVA [5] by 0.5 db or ore [6]. For turbo code, thi can be very iportant, ince the firt decoding iteration can yield 49. Poor error perforance: The ipleentation of the MAP algorith proceed oewhat lie perforing a Viterbi algorith in two direction over a bloc of code bit. Once thi bidirectional coputation yield tate and branch etric for the bloc, the APP and the MAP can be obtained for each data bit repreented within the bloc. The oft-input/oft-output (SISO) decoder i the critical part of the decoder, uing the oft output Viterbi algorith (SOVA) [5], [7] or the log-axiu a poteriori algorith (log-map) [7]. Log-MAP give better perforance than SOVA, but SOVA ha leer coplexe. For real tie application, we want the lowet BER, while latency i not a priority. The MAP algorith i not conidered becaue it ha high coplexity and uffer fro uerical proble. For an encoder eory M=3 the nuber of operation [8] uing MAP, Log-MAP and SOVA. The Log-MAP i.8tie ore coplex than SOVA. Thu, fro a latency point of view SOVA i bet of MAP turbo decoding algorith, for a perforance of view Log-MAP i the bet.the perforance of both algorith for the tandard rate / four tate yteatic convolutional code (g = 7 and g = 5) i given in Table. The BER value for both cae are decreaed, when SR i increaed. Table BER for a four tate code uing MAP decoder & SOVA decoder Eb/0(dB) Log-MAP SOVA Fig 0 Perforance by Siulation of Length 04, Rate / and GeneratorPolynoial G = {7,5}, Turbo Code over AWG Channel. 8 jace, Vol.3, 07 Iterative Decoding of Turbo Code

15 5. Reult A four tate, rate/, 400- bit perforance over the AWG channel after 5 Iteration, we get BER zero when E b / 0 i ore than db in SOVA decoder and.75db in Log-MAP decoder.at the ae bit rate /, 04 perforance over AWG channel after five iteration the Log-MAP decoder how the better perforance than SOVA decoder.at the ae bit rate /3, 04 perforance over AWG channel after five iteration the Log-MAP decoder how earlier BER zero than that of SOVA decoder. 6. Concluion Fro latency point of view, SOVA decoder i better, a it i le coplex, than Log-MAP decoder. On the other hand, the perforance of Log-MAP decoder i ore ound than SOVA decoder. But it i ore coplex than SOVA. 7. Recoendation Reearch on the optiu decoding trategie of the MAP decoder and SOVA decoder over the Raleigh Channel i recoended. Reference. Berrou G., Glavieuc A., and Thitajhia P., ear Shannon liit error-coding: Turbo code, in proc.993, int. conf. co., Geneva, Seitzerland, May 993,pp Bahl L R., Coce J., Jeline F., and Racic J., Optial decoding of linear code for iniizing ybol error rate, IEEE Tran, Infor. Theory, Vol, IT-0, pp, 84-87, Benedetto S., Divalar D., Montori G., and Pollara F., A oft-input oft-output Maxiu A poteriori (MAP) odule to decode parallel and erial concatenated code,tda progre report 4-7, oveber 5, Eroz Mutafa, Roger Haon A. Jr., On the deign of prunableinterleaver for Turbo code, in proc. IEEE VTC 99, Houton, TX, May 5-9, Ungerboec G., Channel Coding with Multilevel/phae Syte, IEEE Tran, on inforation Theory, vol, 8no,, pp, 55-67, January Berrou C. and Glavieux A., Reflection on the prize paper: ear Optiu error correctin coding and decoding turbo code, IEEE Inforation Theory Society ewletter, vol. 48 no., june Perez L., Sgher J., and Cotello D., A Ditance Spectru Interpretation of turbo Code, IEEE Tranaction on Inforation Theory, vol, 4, 6, pp, , ov, Barbulecu A. S. and Pietrobon S.S., On terinating the trelli of Turbo Code in the Sae State, IEE Electronic Letter, vol.3, no. I, Jan Blacert W. J., Hall E. K., and Wilon S. G., Turbo Code Terination and InterleaverConditon, IEE Electronic Letter, vol, 3, no. 4, pp, , ov Slar B., Digital Counication: Fundaental and Application, Chapter 6, Prentice- Hall International, Inc Viterbi A.J, Convolutional Code and their perforance in Counication Syte. IEEE Tran Counication Technology, vol.co-9, no.5, pp 75-77, October 97.. Hagenauer J., Hoeher P., A Viterbi Algorith with Soft-Deciion Output and it Application, proc. GLOBECOM 89, Dalla, Texa, oveber 989, pp Pietrobon S.S., Ipleentation and perforance of a Turbo/MAP decoder, Int t, J Satellite Counication vol. 5, Jan-Feb 998, pp jace, Vol.3, 07 Iterative Decoding of Turbo Code

16 4. Slar B., Digital Counication Fundaental and Application, Second Edition (Upper Saddle River, J: Prentice-Hall, 00) 5. Roberton P., Villebru E., and Hoeher P., A Coparion of Optial and Sub-Optial MAP Decoding Algorith Operating in the Log Doain, proc, of ICC 98, Seattle, Wahington, June 995, pp, Berrou C., Glavieux A., ear Optiu Error Correcting Coding and Decoding Turbo Code, IEEE Tran. On Counication, vol. 44, no. 0, October 99, pp Roberton P., Hoeher P., and Villbrun E., Optial and Sub-Optial MAP Algorith Suitable for Turbo Decoding,Europeon Tranaction on Telecounication. Vol.8, no., pp, 9-5, March-April 997, paper ued in writing Yor turbo coder. 8. Jung P., Coparion of Turbo Code Decoder Applied to Short Frae Traniion, IEEE Journal on elected Area in Counication, vol. 4, no.3, pp, , April Roberton P., Iproving Decoder and Code Structure of Parallel Concatenated Recurive Syteatic (Turbo) Code, in IEE Tran of International Conference on Univeral Peronal Counication, San Diego, Sept. 994, pp, Hagenauer J., Roberton P., and Pape L., Iterative (Turbo) Decoding of Syteatic Convolutional Code with the MAP and SOVA Algorith, in ITG-Fachbericht 30, Oct 994, pp, -9.. Erfanin J., Paupathy S., and Gula G., Reduced Coplexity ybol Detector with Parallel Structure for ISI Channel, IEEE Tran Counication, vol.4, pp , Feb, Mar. Apr Koch W. and Baier A., Optiu and Sub=Optiu Detection of Coded Data Diturbed by Tie Varying ISI, in proceeding GLOBECOM 90, San Diego, Dec.990, pp Roberton P., Illuinating the Structure of Code and Decoder for parallel Concatenated Recurive Syteatic (Turbo) Code, in proceeding of GLOBECOM 94, San Francico, Deceber 994, pp Woodard J.P. and Hanzo L., Coparative Study of Turbo Decoding Technique: An overview, IEEE Tran, on vehicular Technology, ov. 000, vol. 49, o. 6, pp jace, Vol.3, 07 Iterative Decoding of Turbo Code

A Study on Simulating Convolutional Codes and Turbo Codes

A Study on Simulating Convolutional Codes and Turbo Codes A Study on Simulating Convolutional Code and Turbo Code Final Report By Daniel Chang July 27, 2001 Advior: Dr. P. Kinman Executive Summary Thi project include the deign of imulation of everal convolutional

More information

Maximum a Posteriori Decoding of Turbo Codes

Maximum a Posteriori Decoding of Turbo Codes Maxiu a Posteriori Decoing of Turbo Coes by Bernar Slar Introuction The process of turbo-coe ecoing starts with the foration of a posteriori probabilities (APPs) for each ata bit, which is followe by choosing

More information

Jul 4, 2005 turbo_code_primer Revision 0.0. Turbo Code Primer

Jul 4, 2005 turbo_code_primer Revision 0.0. Turbo Code Primer Jul 4, 5 turbo_code_primer Reviion. Turbo Code Primer. Introduction Thi document give a quick tutorial on MAP baed turbo coder. Section develop the background theory. Section work through a imple numerical

More information

HIGH-THROUGHPUT DUAL-MODE SINGLE/DOUBLE BINARY MAP PROCESSOR DESIGN FOR WIRELESS WAN

HIGH-THROUGHPUT DUAL-MODE SINGLE/DOUBLE BINARY MAP PROCESSOR DESIGN FOR WIRELESS WAN HIGH-THROUGHPUT DUAL-MODE SINGLE/DOUBLE BINARY MAP PROCESSOR DESIGN FOR WIRELESS WAN Chun-Yu Chen Cheng-Hung Lin and An-Yeu (Andy) Wu Graduate Intitute of Electronic Engineering and Departent of Electrical

More information

The Extended Balanced Truncation Algorithm

The Extended Balanced Truncation Algorithm International Journal of Coputing and Optiization Vol. 3, 2016, no. 1, 71-82 HIKARI Ltd, www.-hikari.co http://dx.doi.org/10.12988/ijco.2016.635 The Extended Balanced Truncation Algorith Cong Huu Nguyen

More information

A Comparison of Soft In/Soft Out Algorithms for Turbo Detection

A Comparison of Soft In/Soft Out Algorithms for Turbo Detection A Comparion of Soft In/Soft Out Algorithm for Turbo Detection Gerhard Bauch 1, Volker Franz 2 1 Munich Univerity of Technology (TUM), Intitute for Communication Engineering (LNT) D-80290 Munich, Germany

More information

Scale Efficiency in DEA and DEA-R with Weight Restrictions

Scale Efficiency in DEA and DEA-R with Weight Restrictions Available online at http://ijdea.rbiau.ac.ir Int. J. Data Envelopent Analyi (ISSN 2345-458X) Vol.2, No.2, Year 2014 Article ID IJDEA-00226, 5 page Reearch Article International Journal of Data Envelopent

More information

On the Use of High-Order Moment Matching to Approximate the Generalized-K Distribution by a Gamma Distribution

On the Use of High-Order Moment Matching to Approximate the Generalized-K Distribution by a Gamma Distribution On the Ue of High-Order Moent Matching to Approxiate the Generalized- Ditribution by a Gaa Ditribution Saad Al-Ahadi Departent of Syte & Coputer Engineering Carleton Univerity Ottawa Canada aahadi@ce.carleton.ca

More information

Mobile Communications TCS 455

Mobile Communications TCS 455 Mobile Counication TCS 455 Dr. Prapun Sukopong prapun@iit.tu.ac.th Lecture 24 1 Office Hour: BKD 3601-7 Tueday 14:00-16:00 Thurday 9:30-11:30 Announceent Read Chapter 9: 9.1 9.5 Section 1.2 fro [Bahai,

More information

Image Denoising Based on Non-Local Low-Rank Dictionary Learning

Image Denoising Based on Non-Local Low-Rank Dictionary Learning Advanced cience and Technology Letter Vol.11 (AT 16) pp.85-89 http://dx.doi.org/1.1457/atl.16. Iage Denoiing Baed on Non-Local Low-Rank Dictionary Learning Zhang Bo 1 1 Electronic and Inforation Engineering

More information

THE BICYCLE RACE ALBERT SCHUELLER

THE BICYCLE RACE ALBERT SCHUELLER THE BICYCLE RACE ALBERT SCHUELLER. INTRODUCTION We will conider the ituation of a cyclit paing a refrehent tation in a bicycle race and the relative poition of the cyclit and her chaing upport car. The

More information

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog Chapter Sampling and Quantization.1 Analog and Digital Signal In order to invetigate ampling and quantization, the difference between analog and digital ignal mut be undertood. Analog ignal conit of continuou

More information

Turbo Codes. Manjunatha. P. Professor Dept. of ECE. June 29, J.N.N. College of Engineering, Shimoga.

Turbo Codes. Manjunatha. P. Professor Dept. of ECE. June 29, J.N.N. College of Engineering, Shimoga. Turbo Codes Manjunatha. P manjup.jnnce@gmail.com Professor Dept. of ECE J.N.N. College of Engineering, Shimoga June 29, 2013 [1, 2, 3, 4, 5, 6] Note: Slides are prepared to use in class room purpose, may

More information

Lecture 2 DATA ENVELOPMENT ANALYSIS - II

Lecture 2 DATA ENVELOPMENT ANALYSIS - II Lecture DATA ENVELOPMENT ANALYSIS - II Learning objective To eplain Data Envelopent Anali for ultiple input and ultiple output cae in the for of linear prograing .5 DEA: Multiple input, ultiple output

More information

Source slideplayer.com/fundamentals of Analytical Chemistry, F.J. Holler, S.R.Crouch. Chapter 6: Random Errors in Chemical Analysis

Source slideplayer.com/fundamentals of Analytical Chemistry, F.J. Holler, S.R.Crouch. Chapter 6: Random Errors in Chemical Analysis Source lideplayer.com/fundamental of Analytical Chemitry, F.J. Holler, S.R.Crouch Chapter 6: Random Error in Chemical Analyi Random error are preent in every meaurement no matter how careful the experimenter.

More information

ARTICLE IN PRESS. Murat Hüsnü Sazlı a,,canişık b. Syracuse, NY 13244, USA

ARTICLE IN PRESS. Murat Hüsnü Sazlı a,,canişık b. Syracuse, NY 13244, USA S1051-200406)00002-9/FLA AID:621 Vol ) [+odel] P1 1-7) YDSPR:3SC+ v 153 Prn:13/02/2006; 15:33 ydspr621 by:laurynas p 1 Digital Signal Processing ) wwwelsevierco/locate/dsp Neural network ipleentation of

More information

Lecture 2 Phys 798S Spring 2016 Steven Anlage. The heart and soul of superconductivity is the Meissner Effect. This feature uniquely distinguishes

Lecture 2 Phys 798S Spring 2016 Steven Anlage. The heart and soul of superconductivity is the Meissner Effect. This feature uniquely distinguishes ecture Phy 798S Spring 6 Steven Anlage The heart and oul of uperconductivity i the Meiner Effect. Thi feature uniquely ditinguihe uperconductivity fro any other tate of atter. Here we dicu oe iple phenoenological

More information

Ranking DEA Efficient Units with the Most Compromising Common Weights

Ranking DEA Efficient Units with the Most Compromising Common Weights The Sixth International Sypoiu on Operation Reearch and It Application ISORA 06 Xiniang, China, Augut 8 12, 2006 Copyright 2006 ORSC & APORC pp. 219 234 Ranking DEA Efficient Unit with the Mot Coproiing

More information

Chapter 5 Optimum Receivers for the Additive White Gaussian Noise Channel

Chapter 5 Optimum Receivers for the Additive White Gaussian Noise Channel Chapter 5 Optimum Receiver for the Additive White Gauian Noie Channel Table of Content 5.1 Optimum Receiver for Signal Corrupted by Additive White Noie 5.1.1 Correlation Demodulator 5.1. Matched-Filter

More information

Convolutional Codes. Lecture Notes 8: Trellis Codes. Example: K=3,M=2, rate 1/2 code. Figure 95: Convolutional Encoder

Convolutional Codes. Lecture Notes 8: Trellis Codes. Example: K=3,M=2, rate 1/2 code. Figure 95: Convolutional Encoder Convolutional Codes Lecture Notes 8: Trellis Codes In this lecture we discuss construction of signals via a trellis. That is, signals are constructed by labeling the branches of an infinite trellis with

More information

A Genetic Algorithm for Designing Constellations with Low Error Floors

A Genetic Algorithm for Designing Constellations with Low Error Floors A Genetic Algorithm for Deigning Contellation with Low Error Floor Matthew C. Valenti and Raghu Doppalapudi Wet Virginia Univerity Morgantown, WV Email: {mvalenti,doppala}@cee.wvu.edu Don Torrieri U.S.

More information

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281 72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition

More information

Clustering Methods without Given Number of Clusters

Clustering Methods without Given Number of Clusters Clutering Method without Given Number of Cluter Peng Xu, Fei Liu Introduction A we now, mean method i a very effective algorithm of clutering. It mot powerful feature i the calability and implicity. However,

More information

Conservation of Energy

Conservation of Energy Add Iportant Conervation of Energy Page: 340 Note/Cue Here NGSS Standard: HS-PS3- Conervation of Energy MA Curriculu Fraework (006):.,.,.3 AP Phyic Learning Objective: 3.E.., 3.E.., 3.E..3, 3.E..4, 4.C..,

More information

ADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR

ADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR ADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR SAEED ABAZARI MOHSEN HEIDARI NAVID REZA ABJADI Key word: Adaptive control Lyapunov tability Tranient tability Mechanical power. The operating point of

More information

Topic 7 Fuzzy expert systems: Fuzzy inference

Topic 7 Fuzzy expert systems: Fuzzy inference Topic 7 Fuzzy expert yte: Fuzzy inference adani fuzzy inference ugeno fuzzy inference Cae tudy uary Fuzzy inference The ot coonly ued fuzzy inference technique i the o-called adani ethod. In 975, Profeor

More information

SIMM Method Based on Acceleration Extraction for Nonlinear Maneuvering Target Tracking

SIMM Method Based on Acceleration Extraction for Nonlinear Maneuvering Target Tracking Journal of Electrical Engineering & Technology Vol. 7, o. 2, pp. 255~263, 202 255 http://dx.doi.org/0.5370/jeet.202.7.2.255 SIMM Method Baed on Acceleration Extraction for onlinear Maneuvering Target Tracking

More information

ANALOG REALIZATIONS OF FRACTIONAL-ORDER INTEGRATORS/DIFFERENTIATORS A Comparison

ANALOG REALIZATIONS OF FRACTIONAL-ORDER INTEGRATORS/DIFFERENTIATORS A Comparison AALOG REALIZATIOS OF FRACTIOAL-ORDER ITEGRATORS/DIFFERETIATORS A Coparion Guido DEESD, Technical Univerity of Bari, Via de Gaperi, nc, I-7, Taranto, Italy gaione@poliba.it Keyword: Abtract: on-integer-order

More information

Convergence of a Fixed-Point Minimum Error Entropy Algorithm

Convergence of a Fixed-Point Minimum Error Entropy Algorithm Entropy 05, 7, 5549-5560; doi:0.3390/e7085549 Article OPE ACCESS entropy ISS 099-4300 www.dpi.co/journal/entropy Convergence of a Fixed-Point Miniu Error Entropy Algorith Yu Zhang, Badong Chen, *, Xi Liu,

More information

Section J8b: FET Low Frequency Response

Section J8b: FET Low Frequency Response ection J8b: FET ow Frequency epone In thi ection of our tudie, we re o to reiit the baic FET aplifier confiuration but with an additional twit The baic confiuration are the ae a we etiated ection J6 of

More information

DIFFERENTIAL EQUATIONS

DIFFERENTIAL EQUATIONS Matheatic Reviion Guide Introduction to Differential Equation Page of Author: Mark Kudlowki MK HOME TUITION Matheatic Reviion Guide Level: A-Level Year DIFFERENTIAL EQUATIONS Verion : Date: 3-4-3 Matheatic

More information

Lecture 17: Frequency Response of Amplifiers

Lecture 17: Frequency Response of Amplifiers ecture 7: Frequency epone of Aplifier Gu-Yeon Wei Diiion of Engineering and Applied Science Harard Unierity guyeon@eec.harard.edu Wei Oeriew eading S&S: Chapter 7 Ski ection ince otly decribed uing BJT

More information

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays Gain and Phae Margin Baed Delay Dependent Stability Analyi of Two- Area LFC Sytem with Communication Delay Şahin Sönmez and Saffet Ayaun Department of Electrical Engineering, Niğde Ömer Halidemir Univerity,

More information

CHAPTER 13 FILTERS AND TUNED AMPLIFIERS

CHAPTER 13 FILTERS AND TUNED AMPLIFIERS HAPTE FILTES AND TUNED AMPLIFIES hapter Outline. Filter Traniion, Type and Specification. The Filter Tranfer Function. Butterworth and hebyhev Filter. Firt Order and Second Order Filter Function.5 The

More information

24P 2, where W (measuring tape weight per meter) = 0.32 N m

24P 2, where W (measuring tape weight per meter) = 0.32 N m Ue of a 1W Laer to Verify the Speed of Light David M Verillion PHYS 375 North Carolina Agricultural and Technical State Univerity February 3, 2018 Abtract The lab wa et up to verify the accepted value

More information

LEARNING DISCRIMINATIVE BASIS COEFFICIENTS FOR EIGENSPACE MLLR UNSUPERVISED ADAPTATION. Yajie Miao, Florian Metze, Alex Waibel

LEARNING DISCRIMINATIVE BASIS COEFFICIENTS FOR EIGENSPACE MLLR UNSUPERVISED ADAPTATION. Yajie Miao, Florian Metze, Alex Waibel LEARNING DISCRIMINATIVE BASIS COEFFICIENTS FOR EIGENSPACE MLLR UNSUPERVISED ADAPTATION Yajie Miao, Florian Metze, Alex Waibel Language Technologie Intitute, Carnegie Mellon Univerity, Pittburgh, PA, USA

More information

2FSK-LFM Compound Signal Parameter Estimation Based on Joint FRFT-ML Method

2FSK-LFM Compound Signal Parameter Estimation Based on Joint FRFT-ML Method International Conerence on et eaureent Coputational ethod (C 5 FS-F Copound Signal Paraeter Etiation Baed on Joint FF- ethod Zhaoyang Qiu Bin ang School o Electronic Engineering Univerity o Electronic

More information

1-D SEDIMENT NUMERICAL MODEL AND ITS APPLICATION. Weimin Wu 1 and Guolu Yang 2

1-D SEDIMENT NUMERICAL MODEL AND ITS APPLICATION. Weimin Wu 1 and Guolu Yang 2 U-CHINA WORKHOP ON ADVANCED COMPUTATIONAL MODELLING IN HYDROCIENCE & ENGINEERING epteber 9-, Oxford, Miiippi, UA -D EDIMENT NUMERICAL MODEL AND IT APPLICATION Weiin Wu and Guolu Yang ABTRACT A one dienional

More information

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004 18.997 Topic in Combinatorial Optimization April 29th, 2004 Lecture 21 Lecturer: Michel X. Goeman Scribe: Mohammad Mahdian 1 The Lovaz plitting-off lemma Lovaz plitting-off lemma tate the following. Theorem

More information

Chemistry I Unit 3 Review Guide: Energy and Electrons

Chemistry I Unit 3 Review Guide: Energy and Electrons Cheitry I Unit 3 Review Guide: Energy and Electron Practice Quetion and Proble 1. Energy i the capacity to do work. With reference to thi definition, decribe how you would deontrate that each of the following

More information

PHYSICS 211 MIDTERM II 12 May 2004

PHYSICS 211 MIDTERM II 12 May 2004 PHYSIS IDTER II ay 004 Exa i cloed boo, cloed note. Ue only your forula heet. Write all wor and anwer in exa boolet. The bac of page will not be graded unle you o requet on the front of the page. Show

More information

MODE SHAPE EXPANSION FROM DATA-BASED SYSTEM IDENTIFICATION PROCEDURES

MODE SHAPE EXPANSION FROM DATA-BASED SYSTEM IDENTIFICATION PROCEDURES Mecánica Coputacional Vol XXV, pp. 1593-1602 Alberto Cardona, Norberto Nigro, Victorio Sonzogni, Mario Storti. (Ed.) Santa Fe, Argentina, Noviebre 2006 MODE SHAPE EXPANSION FROM DATA-BASED SYSTEM IDENTIFICATION

More information

Lecture 10 Filtering: Applied Concepts

Lecture 10 Filtering: Applied Concepts Lecture Filtering: Applied Concept In the previou two lecture, you have learned about finite-impule-repone (FIR) and infinite-impule-repone (IIR) filter. In thee lecture, we introduced the concept of filtering

More information

An Exact Solution for the Deflection of a Clamped Rectangular Plate under Uniform Load

An Exact Solution for the Deflection of a Clamped Rectangular Plate under Uniform Load Applied Matheatical Science, Vol. 1, 007, no. 3, 19-137 An Exact Solution for the Deflection of a Claped Rectangular Plate under Unifor Load C.E. İrak and İ. Gerdeeli Itanbul Technical Univerity Faculty

More information

Codes Correcting Two Deletions

Codes Correcting Two Deletions 1 Code Correcting Two Deletion Ryan Gabry and Frederic Sala Spawar Sytem Center Univerity of California, Lo Angele ryan.gabry@navy.mil fredala@ucla.edu Abtract In thi work, we invetigate the problem of

More information

A First Digit Theorem for Square-Free Integer Powers

A First Digit Theorem for Square-Free Integer Powers Pure Matheatical Science, Vol. 3, 014, no. 3, 19-139 HIKARI Ltd, www.-hikari.co http://dx.doi.org/10.1988/p.014.4615 A Firt Digit Theore or Square-Free Integer Power Werner Hürliann Feldtrae 145, CH-8004

More information

Bayesian Reliability Estimation of Inverted Exponential Distribution under Progressive Type-II Censored Data

Bayesian Reliability Estimation of Inverted Exponential Distribution under Progressive Type-II Censored Data J. Stat. Appl. Pro. 3, No. 3, 317-333 (2014) 317 Journal of Statitic Application & Probability An International Journal http://dx.doi.org/10.12785/jap/030303 Bayeian Reliability Etiation of Inverted Exponential

More information

4.5 Evaporation and Diffusion Evaporation and Diffusion through Quiescent Air (page 286) bulk motion of air and j. y a,2, y j,2 or P a,2, P j,2

4.5 Evaporation and Diffusion Evaporation and Diffusion through Quiescent Air (page 286) bulk motion of air and j. y a,2, y j,2 or P a,2, P j,2 4.5 Evaporation and Diffuion 4.5.4 Evaporation and Diffuion through Quiecent Air (page 86) z bul otion of air and j z diffuion of air (a) diffuion of containant (j) y a,, y j, or P a,, P j, z 1 volatile

More information

_10_EE394J_2_Spring12_Inertia_Calculation.doc. Procedure for Estimating Grid Inertia H from Frequency Droop Measurements

_10_EE394J_2_Spring12_Inertia_Calculation.doc. Procedure for Estimating Grid Inertia H from Frequency Droop Measurements Procedure or Etiating Grid Inertia ro Frequency Droop Meaureent While the exion or inertia and requency droop are well known, it i prudent to rederive the here. Treating all the grid generator a one large

More information

4 Conservation of Momentum

4 Conservation of Momentum hapter 4 oneration of oentu 4 oneration of oentu A coon itake inoling coneration of oentu crop up in the cae of totally inelatic colliion of two object, the kind of colliion in which the two colliding

More information

Problem Set 8 Solutions

Problem Set 8 Solutions Deign and Analyi of Algorithm April 29, 2015 Maachuett Intitute of Technology 6.046J/18.410J Prof. Erik Demaine, Srini Devada, and Nancy Lynch Problem Set 8 Solution Problem Set 8 Solution Thi problem

More information

Design By Emulation (Indirect Method)

Design By Emulation (Indirect Method) Deign By Emulation (Indirect Method he baic trategy here i, that Given a continuou tranfer function, it i required to find the bet dicrete equivalent uch that the ignal produced by paing an input ignal

More information

Performance Analysis of Sub-Rating for Handoff Calls in HCN

Performance Analysis of Sub-Rating for Handoff Calls in HCN I. J. Counication, Network and Syte Science, 29, 1, 1-89 Publihed Online February 29 in SciRe (http://www.scirp.org/journal/ijcn/). Perforance Analyi of Sub-Rating for Handoff Call in HCN Xiaolong WU 1,

More information

Auditorium & Room Acoustics

Auditorium & Room Acoustics UIUC Phyic 406 Acoutical Phyic of Muic Auditoriu & Roo Acoutic Sound out in the open, ditance r away fro ound ource: Free Field r Sound Intenity I () r = Power 4pr ound ource: r Intenity, I in Watt/ (ince

More information

The Features For Dark Matter And Dark Flow Found.

The Features For Dark Matter And Dark Flow Found. The Feature For Dark Matter And Dark Flow Found. Author: Dan Vier, Alere, the Netherland Date: January 04 Abtract. Fly-By- and GPS-atellite reveal an earth-dark atter-halo i affecting the orbit-velocitie

More information

Research Article Efficient Recursive Methods for Partial Fraction Expansion of General Rational Functions

Research Article Efficient Recursive Methods for Partial Fraction Expansion of General Rational Functions Journal of Applied atheatic Volue 24, Article ID 89536, 8 page http://dx.doi.org/.55/24/89536 Reearch Article Efficient Recurive ethod for Partial Fraction Expanion of General Rational Function Youneng

More information

Relevance Estimation of Cooperative Awareness Messages in VANETs

Relevance Estimation of Cooperative Awareness Messages in VANETs Relevance Etiation of Cooperative Awarene Meage in VANET Jakob Breu Reearch and Developent Dailer AG Böblingen, Gerany Eail: jakobbreu@dailerco Michael Menth Departent of Coputer Science Univerity of Tübingen

More information

Bogoliubov Transformation in Classical Mechanics

Bogoliubov Transformation in Classical Mechanics Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How

More information

Control of industrial robots. Decentralized control

Control of industrial robots. Decentralized control Control of indutrial robot Decentralized control Prof Paolo Rocco (paolorocco@poliiit) Politecnico di Milano Dipartiento di Elettronica, Inforazione e Bioingegneria Introduction Once the deired otion of

More information

ECE 3510 Root Locus Design Examples. PI To eliminate steady-state error (for constant inputs) & perfect rejection of constant disturbances

ECE 3510 Root Locus Design Examples. PI To eliminate steady-state error (for constant inputs) & perfect rejection of constant disturbances ECE 350 Root Locu Deign Example Recall the imple crude ervo from lab G( ) 0 6.64 53.78 σ = = 3 23.473 PI To eliminate teady-tate error (for contant input) & perfect reection of contant diturbance Note:

More information

LOAD AND RESISTANCE FACTOR DESIGN APPROACH FOR FATIGUE OF MARINE STRUCTURES

LOAD AND RESISTANCE FACTOR DESIGN APPROACH FOR FATIGUE OF MARINE STRUCTURES 8 th ACE pecialty Conference on Probabilitic Mechanic and tructural Reliability PMC2000-169 LOAD AND REITANCE FACTOR DEIGN APPROACH FOR FATIGUE OF MARINE TRUCTURE Abtract I.A. Aakkaf, G. ACE, and B.M.

More information

On Constant Power Water-filling

On Constant Power Water-filling On Constant Power Water-filling Wei Yu and John M. Cioffi Electrical Engineering Departent Stanford University, Stanford, CA94305, U.S.A. eails: {weiyu,cioffi}@stanford.edu Abstract This paper derives

More information

Suggested Answers To Exercises. estimates variability in a sampling distribution of random means. About 68% of means fall

Suggested Answers To Exercises. estimates variability in a sampling distribution of random means. About 68% of means fall Beyond Significance Teting ( nd Edition), Rex B. Kline Suggeted Anwer To Exercie Chapter. The tatitic meaure variability among core at the cae level. In a normal ditribution, about 68% of the core fall

More information

Hybrid technique based on chirp effect and phase shifts for spectral Talbot effect in sampled fiber Bragg gratings (FBGs)

Hybrid technique based on chirp effect and phase shifts for spectral Talbot effect in sampled fiber Bragg gratings (FBGs) Optica Applicata, Vol. XLI, No. 1, 011 Hybrid technique baed on chirp effect and phae hift for pectral Talbot effect in apled fiber Bragg grating (FBG) GUO DENG *, WEI PAN Center for Inforation Photonic

More information

Social Studies 201 Notes for November 14, 2003

Social Studies 201 Notes for November 14, 2003 1 Social Studie 201 Note for November 14, 2003 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the

More information

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment

Advanced D-Partitioning Analysis and its Comparison with the Kharitonov s Theorem Assessment Journal of Multidiciplinary Engineering Science and Technology (JMEST) ISSN: 59- Vol. Iue, January - 5 Advanced D-Partitioning Analyi and it Comparion with the haritonov Theorem Aement amen M. Yanev Profeor,

More information

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems

A Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems A Contraint Propagation Algorithm for Determining the Stability Margin of Linear Parameter Circuit and Sytem Lubomir Kolev and Simona Filipova-Petrakieva Abtract The paper addree the tability margin aement

More information

1. The F-test for Equality of Two Variances

1. The F-test for Equality of Two Variances . The F-tet for Equality of Two Variance Previouly we've learned how to tet whether two population mean are equal, uing data from two independent ample. We can alo tet whether two population variance are

More information

Persistent Spread Measurement for Big Network Data Based on Register Intersection

Persistent Spread Measurement for Big Network Data Based on Register Intersection Peritent Spread Meaureent for Big Network Data Baed on Regiter Interection YOU ZHOU, Univerity of Florida YIAN ZHOU, Google Inc. and Univerity of Florida MIN CHEN, Google Inc. and Univerity of Florida

More information

Comparing Means: t-tests for Two Independent Samples

Comparing Means: t-tests for Two Independent Samples Comparing ean: t-tet for Two Independent Sample Independent-eaure Deign t-tet for Two Independent Sample Allow reearcher to evaluate the mean difference between two population uing data from two eparate

More information

Performance Analysis of a Three-Channel Control Architecture for Bilateral Teleoperation with Time Delay

Performance Analysis of a Three-Channel Control Architecture for Bilateral Teleoperation with Time Delay Extended Suary pp.1224 1230 Perforance Analyi of a Three-Channel Control Architecture for Bilateral Teleoperation with Tie Delay Ryogo Kubo Meber (Keio Univerity, kubo@u.d.keio.ac.jp) Noriko Iiyaa Student

More information

Social Studies 201 Notes for March 18, 2005

Social Studies 201 Notes for March 18, 2005 1 Social Studie 201 Note for March 18, 2005 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the

More information

The Influence of the Load Condition upon the Radial Distribution of Electromagnetic Vibration and Noise in a Three-Phase Squirrel-Cage Induction Motor

The Influence of the Load Condition upon the Radial Distribution of Electromagnetic Vibration and Noise in a Three-Phase Squirrel-Cage Induction Motor The Influence of the Load Condition upon the Radial Ditribution of Electromagnetic Vibration and Noie in a Three-Phae Squirrel-Cage Induction Motor Yuta Sato 1, Iao Hirotuka 1, Kazuo Tuboi 1, Maanori Nakamura

More information

Z a>2 s 1n = X L - m. X L = m + Z a>2 s 1n X L = The decision rule for this one-tail test is

Z a>2 s 1n = X L - m. X L = m + Z a>2 s 1n X L = The decision rule for this one-tail test is M09_BERE8380_12_OM_C09.QD 2/21/11 3:44 PM Page 1 9.6 The Power of a Tet 9.6 The Power of a Tet 1 Section 9.1 defined Type I and Type II error and their aociated rik. Recall that a repreent the probability

More information

Related Rates section 3.9

Related Rates section 3.9 Related Rate ection 3.9 Iportant Note: In olving the related rate proble, the rate of change of a quantity i given and the rate of change of another quantity i aked for. You need to find a relationhip

More information

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}

More information

TP A.30 The effect of cue tip offset, cue weight, and cue speed on cue ball speed and spin

TP A.30 The effect of cue tip offset, cue weight, and cue speed on cue ball speed and spin technical proof TP A.30 The effect of cue tip offet, cue weight, and cue peed on cue all peed and pin technical proof upporting: The Illutrated Principle of Pool and Billiard http://illiard.colotate.edu

More information

Lecture 4 Topic 3: General linear models (GLMs), the fundamentals of the analysis of variance (ANOVA), and completely randomized designs (CRDs)

Lecture 4 Topic 3: General linear models (GLMs), the fundamentals of the analysis of variance (ANOVA), and completely randomized designs (CRDs) Lecture 4 Topic 3: General linear model (GLM), the fundamental of the analyi of variance (ANOVA), and completely randomized deign (CRD) The general linear model One population: An obervation i explained

More information

THE PARAMETERIZATION OF ALL TWO-DEGREES-OF-FREEDOM SEMISTRONGLY STABILIZING CONTROLLERS. Tatsuya Hoshikawa, Kou Yamada and Yuko Tatsumi

THE PARAMETERIZATION OF ALL TWO-DEGREES-OF-FREEDOM SEMISTRONGLY STABILIZING CONTROLLERS. Tatsuya Hoshikawa, Kou Yamada and Yuko Tatsumi International Journal of Innovative Computing, Information Control ICIC International c 206 ISSN 349-498 Volume 2, Number 2, April 206 pp. 357 370 THE PARAMETERIZATION OF ALL TWO-DEGREES-OF-FREEDOM SEMISTRONGLY

More information

S E V E N. Steady-State Errors SOLUTIONS TO CASE STUDIES CHALLENGES

S E V E N. Steady-State Errors SOLUTIONS TO CASE STUDIES CHALLENGES S E V E N Steady-State Error SOLUTIONS TO CASE STUDIES CHALLENGES Antenna Control: Steady-State Error Deign via Gain 76.39 a. G( (50)(.3). Syte i Type. Step input: e( ) 0; Rap input: e( ) v 76.39.59 ;

More information

What lies between Δx E, which represents the steam valve, and ΔP M, which is the mechanical power into the synchronous machine?

What lies between Δx E, which represents the steam valve, and ΔP M, which is the mechanical power into the synchronous machine? A 2.0 Introduction In the lat et of note, we developed a model of the peed governing mechanim, which i given below: xˆ K ( Pˆ ˆ) E () In thee note, we want to extend thi model o that it relate the actual

More information

PPP AND UNIT ROOTS: LEARNING ACROSS REGIMES

PPP AND UNIT ROOTS: LEARNING ACROSS REGIMES PPP AND UNIT ROOTS: LEARNING ACROSS REGIMES GERALD P. DYWER, MARK FISHER, THOMAS J. FLAVIN, AND JAMES R. LOTHIAN Preliinary and incoplete Abtract. Taking a Bayeian approach, we focu on the inforation content

More information

Predicting the Performance of Teams of Bounded Rational Decision-makers Using a Markov Chain Model

Predicting the Performance of Teams of Bounded Rational Decision-makers Using a Markov Chain Model The InTITuTe for ytem reearch Ir TechnIcal report 2013-14 Predicting the Performance of Team of Bounded Rational Deciion-maer Uing a Marov Chain Model Jeffrey Herrmann Ir develop, applie and teache advanced

More information

Fading Channels: Capacity, BER and Diversity

Fading Channels: Capacity, BER and Diversity Fading Channel: Capacity, BER and Diverity Mater Univeritario en Ingeniería de Telecomunicación I. Santamaría Univeridad de Cantabria Introduction Capacity BER Diverity Concluion Content Introduction Capacity

More information

μ + = σ = D 4 σ = D 3 σ = σ = All units in parts (a) and (b) are in V. (1) x chart: Center = μ = 0.75 UCL =

μ + = σ = D 4 σ = D 3 σ = σ = All units in parts (a) and (b) are in V. (1) x chart: Center = μ = 0.75 UCL = Our online Tutor are available 4*7 to provide Help with Proce control ytem Homework/Aignment or a long term Graduate/Undergraduate Proce control ytem Project. Our Tutor being experienced and proficient

More information

Question 1 Equivalent Circuits

Question 1 Equivalent Circuits MAE 40 inear ircuit Fall 2007 Final Intruction ) Thi exam i open book You may ue whatever written material you chooe, including your cla note and textbook You may ue a hand calculator with no communication

More information

Nonlinear BCJR equalizer for suppression of intrachannel nonlinearities in 40 Gb/s optical communications systems

Nonlinear BCJR equalizer for suppression of intrachannel nonlinearities in 40 Gb/s optical communications systems Nonlinear BCJR equalizer for uppreion of intrachannel nonlinearitie in 40 Gb/ optical communication ytem Ivan B. Dordevic and Bane Vaic Univerity of Arizona Department of Electrical and Computer Engineering

More information

Adaptive Radar Signal Detection with Integrated Learning and Knowledge Exploitation

Adaptive Radar Signal Detection with Integrated Learning and Knowledge Exploitation Integrated Learning and Knowledge Exploitation Hongbin Li Departent of Electrical and Coputer Engineering Steven Intitute of Technology, Hoboken, NJ 73 USA hli@teven.edu Muralidhar Rangaway AFRL/RYAP Bldg

More information

Practice Problem Solutions. Identify the Goal The acceleration of the object Variables and Constants Known Implied Unknown m = 4.

Practice Problem Solutions. Identify the Goal The acceleration of the object Variables and Constants Known Implied Unknown m = 4. Chapter 5 Newton Law Practice Proble Solution Student Textbook page 163 1. Frae the Proble - Draw a free body diagra of the proble. - The downward force of gravity i balanced by the upward noral force.

More information

Improved Interference Cancellation Scheme for Two-User Detection of Alamouti Code

Improved Interference Cancellation Scheme for Two-User Detection of Alamouti Code Improved Interference Cancellation Scheme for Two-Uer Detection of Alamouti Code Manav R hatnagar and Are Hjørungne Abtract In thi correpondence, we propoe an improved interference cancellation method

More information

m 0 are described by two-component relativistic equations. Accordingly, the noncharged

m 0 are described by two-component relativistic equations. Accordingly, the noncharged Generalized Relativitic Equation of Arbitrary Ma and Spin and Bai Set of Spinor Function for It Solution in Poition, Moentu and Four-Dienional Space Abtract I.I.Gueinov Departent of Phyic, Faculty of Art

More information

THE RATIO OF DISPLACEMENT AMPLIFICATION FACTOR TO FORCE REDUCTION FACTOR

THE RATIO OF DISPLACEMENT AMPLIFICATION FACTOR TO FORCE REDUCTION FACTOR 3 th World Conference on Earthquake Engineering Vancouver, B.C., Canada Augut -6, 4 Paper No. 97 THE RATIO OF DISPLACEMENT AMPLIFICATION FACTOR TO FORCE REDUCTION FACTOR Mua MAHMOUDI SUMMARY For Seimic

More information

Vulnerability of MRD-Code-Based Universal Secure Error-Correcting Network Codes under Time-Varying Jamming Links

Vulnerability of MRD-Code-Based Universal Secure Error-Correcting Network Codes under Time-Varying Jamming Links Vulnerability of MRD-Code-Based Universal Secure Error-Correcting Network Codes under Tie-Varying Jaing Links Jun Kurihara KDDI R&D Laboratories, Inc 2 5 Ohara, Fujiino, Saitaa, 356 8502 Japan Eail: kurihara@kddilabsjp

More information

Privacy-Preserving Point-to-Point Transportation Traffic Measurement through Bit Array Masking in Intelligent Cyber-Physical Road Systems

Privacy-Preserving Point-to-Point Transportation Traffic Measurement through Bit Array Masking in Intelligent Cyber-Physical Road Systems Privacy-Preerving Point-to-Point Tranportation Traffic Meaureent through Bit Array Making in Intelligent Cyber-Phyical Road Syte Yian Zhou Qingjun Xiao Zhen Mo Shigang Chen Yafeng Yin Departent of Coputer

More information

III.9. THE HYSTERESIS CYCLE OF FERROELECTRIC SUBSTANCES

III.9. THE HYSTERESIS CYCLE OF FERROELECTRIC SUBSTANCES III.9. THE HYSTERESIS CYCLE OF FERROELECTRIC SBSTANCES. Work purpoe The analyi of the behaviour of a ferroelectric ubtance placed in an eternal electric field; the dependence of the electrical polariation

More information

Fair scheduling in cellular systems in the presence of noncooperative mobiles

Fair scheduling in cellular systems in the presence of noncooperative mobiles 1 Fair cheduling in cellular yte in the preence of noncooperative obile Veeraruna Kavitha +, Eitan Altan R. El-Azouzi + and Rajeh Sundarean Maetro group, INRIA, 2004 Route de Luciole, Sophia Antipoli,

More information

Chapter 7. Principles of Unsteady - State and Convective Mass Transfer

Chapter 7. Principles of Unsteady - State and Convective Mass Transfer Suppleental Material for Tranport Proce and Separation Proce Principle hapter 7 Principle of Unteady - State and onvective Ma Tranfer Thi chapter cover different ituation where a tranfer i taking place,

More information

This model assumes that the probability of a gap has size i is proportional to 1/i. i.e., i log m e. j=1. E[gap size] = i P r(i) = N f t.

This model assumes that the probability of a gap has size i is proportional to 1/i. i.e., i log m e. j=1. E[gap size] = i P r(i) = N f t. CS 493: Algoriths for Massive Data Sets Feb 2, 2002 Local Models, Bloo Filter Scribe: Qin Lv Local Models In global odels, every inverted file entry is copressed with the sae odel. This work wells when

More information

Investigation of application of extractive distillation method in chloroform manufacture

Investigation of application of extractive distillation method in chloroform manufacture Invetigation of application of etractive ditillation ethod in chlorofor anufacture Proceeding of uropean Congre of Cheical ngineering (CC-6) Copenhagen, 16-20 Septeber 2007 Invetigation of application

More information

Unified Model for Short-Channel Poly-Si TFTs

Unified Model for Short-Channel Poly-Si TFTs Unified Model for Short-Channel Poly-Si TFT Benjaín Iñiguez, 1 Zheng Xu, 1 Tor A. Fjeldly 1, and Michael. S. Shur 1 1 Departent of Electrical, Coputer, and Syte Engineering, Renelaer Polytechnic Intitute,

More information