INTERNATIONAL JOURNAL OF COMPUTERS AND COMMUNICATIONS Issue 1, Volume 7, Theoretical Analysis of BER Performance of Optical ZCZ-CDMA System

Size: px
Start display at page:

Download "INTERNATIONAL JOURNAL OF COMPUTERS AND COMMUNICATIONS Issue 1, Volume 7, Theoretical Analysis of BER Performance of Optical ZCZ-CDMA System"

Transcription

1 ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, 3 Thortical Analysis of BER Prformanc of Optical ZCZ-CDMA Systm Takahiro MATSUMOTO, Hidyuki TORII and Shinya MATSUFUJI Abstract In this papr, w analyz th bit rror rat BER prformanc of optical cod division multipl accss CDMA systm basd on th optical zro-corrlation zon ZCZ cod with zrocorrlation zon n or which is calld th optical ZCZ-CDMA systm, by th lctrical and optical procssing ovr th optical fibr and spac by computr and thortical formula. In th optical fibr transmission of this systm, th ffct of th avalanch photodiod APD nois, thrmal nois and co-channl intrfrnc ar considrd. Additionally, th ffcts of th scintillation and background nois ar considrd in th optical spac transmission of this systm. Th optical ZCZ cod, which is a st of pairs of binary and biphas squncs consisting of or with zro-corrlation zon, may b abl to provid optical CDMA communication systm supprssd co-channl intrfrnc, and w hav proposd th compact construction of a cod gnrator and a bank of matchd filtrs for this cod. As a rsult, th BER prformanc of optical ZCZ-CDMA systm ovr th optical spac go down compard to that ovr th optical fibr, and th BER prformanc of this systm by th lctrical procssing go down compard to that by th optical procssing, and this systm can t rmov compltly co-channl intrfrnc. Kywords optical communication, optical cod division multipl accss CDMA, optical ZCZ cod, scintillation, avalanch photodiod APD nois, co-channl intrfrnc. provid optical CDMA communication systm supprssd cochannl intrfrnc [], [], [3], and w hav proposd th compact construction of a cod gnrator [] and a bank of matchd filtrs [5], [6] for this cod. In th low- and hi-spd optical communications, th rcivr is procssd by lctrical and optical signals, rspctivly. Th formr and lattr ar calld th lctrical and optical procssing, rspctivly. Th communication prformanc of this systm is influncd from ths procssing. In this papr, w analyz th bit rror rat BER prformanc of optical CDMA systm basd on th optical ZCZ cod with zro-corrlation zon n or which is calld th optical ZCZ-CDMA systm, by th lctrical and optical procssing ovr th optical fibr and spac by computr and thortical formula. In th optical fibr transmission of this systm, th ffct of th avalanch photodiod APD nois, thrmal nois and co-channl intrfrnc ar considrd. Additionally, in th optical spac transmission of this systm, th ffcts of th scintillation and background nois ar considrd. I. ITRODUCTIO THE optical cod division multipl accss CDMA communication systm can xpct a high spd communication bcaus this systm is abl to us a wid band [], [], [3]. In addition, this systm can giv th multipl accss without changing th wav lngth. In th optical CDMA systm, a psudo-nois P squnc usd to this systm dcids th communication prformanc [], [5], [6], [7], [8], and an optical orthogonal cod is oftn gnrally usd as a P squnc. Th optical orthogonal cod [9] is a st of binary squncs consisting of or, and its crosscorrlation proprty has low corrlation valu. Thrfor, th optical CDMA communication systm basd on optical orthogonal cod gos down th bit rror rat BER prformanc. On th othr hand, th optical zro-corrlation zon ZCZ cod [] is a st of pairs of a binary squnc consisting of or and a biphas squnc consisting of or with zro-corrlation zon. Thrfor, this cod may b abl to Manuscript rcivd Dcmbr 3,. T. Matsumoto is associat profssor with Univrsity Evaluat Dpartmnt, Yamaguchi Univrsity, Yamaguchi-shi, Yamaguchi, Japan -mail: matugn@yamaguchi-u.ac.p. H. Torii is associat profssor with Dpartmnt of Information twork and Communication, Kanagawa Institut of Tchnology, Atsugi-shi, Kanagawa, Japan -mail:torii@nw.kanagawa-it.ac.p. S. Matsufui is profssor with Graduat School of Scinc and Enginring, Yamaguchi Univrsity, Ub-shi, Yamaguchi, Japan -mail: s- matsu@yamaguchi-u.ac.p. 8 II. OPTICAL ZCZ CODE A. Dfinition of optical ZCZ cod Lt a b a biphas squnc of lngth whos lmnts tak or, writtn as a = a,, a,,, a,i,, a,, a,i {,. Similarly, lt â,d b a binary squnc of lngth whos lmnts tak or, writtn as â,d = â,d,, â,d,,, â,d,i,, â,d,, â,d,i {,, d {,, whr i dnots i mod. Lt A b a st of M pairs consisting of a biphas squnc a and a binary squnc â,d, writtn as A = {a, â,d, a, â,d,, a, â,d,, a M, â M,d, 3 whr M is th numbr of squncs in a squnc family and is calld family siz. A priodic corrlation function btwn squncs a and â,d at shift i is dfind by ρ a,â,d,i = a,iâ,d,i+i mod.

2 ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, 3 In this papr, th abov corrlation function ρ a,â,d is,i calld th auto-corrlation function for = and th crosscorrlation function for. Th st is calld an optical ZCZ cod [] if th priodic auto- and cross-corrlation functions satisfy ρ a,â,d,i = w = w ; i =, =, d =, w ; i =, =, d =, ; i =,, ; i z, 5 â,d,i <, 6 whr w is th numbr of th nonzro lmnts in ach squnc and z is a zro-corrlation zon. Th optical ZCZ cods ar boundd by M z +. 7 B. Optical ZCZ cod with z = n Lt b b a Lgndr squnc [9] of lngth = n with positiv n or an M-squnc of lngth = n with n, whos lmnts tak valus of or, writtn as b = b,, b,,, b,i,, b,, 8 b,i {, with b,i =. A binary squnc ˆb,i {, of lngth is givn by ˆb,i = + b,i. 9 On th othr hand, lt H b an Hadamard matrix of ordr = n with n, writtn as H = [h, h,, h,, h ] T, h = h,, h,,, h,,,i h,, h,i {,, whr T dnots th matrix transposition, h is calld an Hadamard squnc and h =, i,i. A binary squnc ĥ,d,i {, of lngth is givn by Lt A b a st of M = pairs consisting of a biphas squnc a and a binary squnc â,d of lngth =, writtn as { A = a, â,d, a, â,d,, a, â,d,, a, â,d. 5 Th priodic corrlation function btwn a and,d â xcpt whn = = is givn by ρ a,â,d,i = + ; i =, =, d =, + ; i =, =, d =, ; i =,, ; i z =, 6 whr / < w = + / /3. Thrfor, th abov st of M = pairs consisting of a biphas squnc a and a binary squnc,d â is an optical ZCZ cod [] with z = = n and M = = /z +. As an xampl, w gnrat an optical ZCZ cod of = = 3 =, z = = and M = = 3. Lt and H = b 3 = +, +, h h h h 3 = , 7 whr H is a Sylvstr-typ Hadamard matrix, + and dnot + and, rspctivly. From Eq. 3, w can gnrat bi-phas squncs a, as follows, rspctivly. Similarly, lt a = +,,,, +, +, +,,,, +, +, a = +, +, +,, +,,,,, +,, +, a 3 = +,, +, +, +, +,, +,,,,. ˆb3 = +, +, ĥ,d,i = + d h,i. If and ar rlativly prim, i.., gcd, =, a biphas squnc a of lngth = is producd by a,i = b,i mod h,i mod. 3 Similarly, a binary squnc â,d of lngth = is producd by â,d,i = ˆb,i mod ĥ,d,i mod. 9 and ĥ, ĥ, ĥ, ĥ 3, ĥ, ĥ, ĥ, ĥ 3, = = ,,

3 ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, 3 3 whr + dnots. From Eq., w can gnrat binary squncs â, as follows, rspctivly. â, = +,,,, +,, +,,,, +,, â, = +, +,,, +,,,,, +,,, â 3, = +,,, +, +,,, +,,,,, â, =, +,, +,,,, +,, +,,, â, =,,, +,,, +, +,,, +,, â 3, =, +,,,,, +,,, +, +,. A st consisting of a bi-phas squnc a and a binary squnc â,d, is an optical ZCZ cod with =, z = and M = 3. Its auto-corrlation functions ar givn by ρ a,â,,i =,,,,,,,,,,,, ρ a,â,,i =,,,,,,,,,,,, ρ a 3,â 3,,i =,,,,,,,,,,,, ρ a,â,,i =,,,,,,,,,,,, ρ a,â,,i =,,,,,,,,,,,, ρ a 3,â 3,,i =,,,,,,,,,,, and its cross-corrlation functions ρ a,â,,i =,,,,,,,,,,,, ρ a,â 3,,i =,,,,,,,,,,,, ρ a 3,â,,i =,,,,,,,,,,,, ρ a,â,,i =,,,,,,,,,,,, ρ a,â 3,,i =,,,,,,,,,,,, ρ a 3,â,,i =,,,,,,,,,,,. C. Optical ZCZ cod with z = Lt S b a Sylvstr-typ Hadamard matrix of ordr = n with n, writtn as S = [s, s,, s,, s ] T, 8 s = s,, s,,, s,,,i s,, 9 s,i {,, whr T dnots th matrix transposition. It can also b xprssd as S = S S, [ ] S =, whr th opration dnots th Kronckr product. Each row s is calld a Sylvstr-typ Hadamard squnc. A biphas squnc a with lngth = is givn by From Eqs. and 3, th man valu of this squnc a is givn by a,i = s,is,i s,is,i =, whr,. Thrfor, a biphas squnc a is calld a biphas balancd squnc. A binary squnc â,d of lngth is givn by â,d,i = + d a,i. 5 Lt A b a st of M = / pairs consisting of a biphas squnc a and a binary squnc â,d of lngth =, writtn as { A = a, â,d, a3, â 3,d,, a, â,d,, a, â,d. 6 Th priodic corrlation function btwn a and,d â xcpt whn, is givn by ρ a,â,d,i = ; i =, =, d =, ; i =, =, d =, ; i =,, ; i = ±z = ±, 7 whr w = /. Thrfor, th abov st of M = / pairs consisting of a biphas squnc a and a binary squnc â,d is an optical ZCZ cod with z = and M = / = /z +. As an xampl, w gnrat an optical ZCZ cod of = = = 8, z = and M = / =. From Eqs. 7, and 3, w can gnrat bi-phas squncs a 8, as follows, rspctivly. a 8 = +, +,,,, +, +,, a 3 8 = +,,, +,,, +, +. From Eq. 5, w can gnrat binary squncs â,d 8, as follows, rspctivly. â, 8 = +, +,,,, +, +,, â 3, 8 = +,,, +,,, +, +, â, 8 =,, +, +, +,,, +, â 3, 8 =, +, +,, +, +,,. A st of pairs consisting of a bi-phas squnc a 8 and a binary squnc â,d 8 is an optical ZCZ cod with = 8, z = and M =. Its auto-corrlation functions ar givn by ρ a 8,â, = ρ 8,i a 3 8,â 3, 8,i =,,,,,,,, ρ a 8,â, = ρ 8,i a 3 8,â 3, 8,i =,,,,,,, a,i = α,i s,i mod, and its cross-corrlation functions ar givn by { s α,i =,i mod = ; i, s,i mod = i+ ; i. ρ a 8,â 3, = ρ 8,i a 3 8,â, =,,,,,,,, 8,i ρ 3 a 8,â 3, = ρ 8,i a 3 8,â, =,,,,,,,. 8,i

4 ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, 3 III. OPTICAL ZCZ-CDMA SYSTEM Th optical CDMA systm basd on th optical ZCZ cod is calld th optical ZCZ-CDMA systm. In th transmittr, th binary squnc is usd to snd optical signal corrsponding to a short puls and th absnc of light. A transmittr snds a binary squnc â,d in according to input data d {, as optical signal. On th othr hand, in th rcivr, th biphas squnc is usd as th rfrnc squnc. In a low-spd communication, th rcivr is procssd by an lctrical signal, which is calld th lctrical procssing. This systm nds on avalanch photodiod APD lmnt. Figur shows optical ZCZ-CDMA systm by th lctrical procssing. Th rcivd signal r i is passd through a filtr matchd to th biphas squnc, a, which is calld th lctrical corrlator, and is rcovrd to th bit data in th dtctor. From Eq., th input of a dtctor R is givn by R = a,i r i. 8 Similarly, in a high-spd communication, th rcivr is procssd by an optical signal, which is calld th optical procssing. This systm nds two avalanch photodiod APD lmnts bcaus th rfrnc squnc is th biphas squnc which taks as or. Figur shows optical ZCZ-CDMA systm by th optical procssing. In splittr, th rcivd signal is switchd to th optical corrlator and according to lmnt valus and of th rfrnc squnc a, rspctivly, and is addd as ˆR and ˆR in th optical corrlator and, rspctivly. Th diffrnc output signal of APD and APD is rcovrd to th bit data in th dtctor. From Eq. 8, th input of a dtctor R is givn by + a,i a,i R = r i r i = ˆR ˆR. 9 ot that if z = thn + a,i / and a,i / ar from Eq. 5, rspctivly. â,,i and â,,i IV. THEORETICAL AALYSIS OF BER PERFORMACE W thortically analys th BER prformanc of optical ZCZ-CDMA systms by th lctrical and optical procssing, and valuat it by computr. Tabl I shows spcifications of thortical analysis and computr. A. BER prformanc in optical fibr transmission Th thortical formula of BER charactristics of th optical ZCZ-CDMA systm by th lctrical procssing ovr th optical fibr is givn by p BER = πσ m = rfc { a µ xp σ da m, 3 µ σ m M µ = wgt c λ s, 3 M TABLE I SPECIFICATIOS OF THEORETICAL AALYSIS AD COMPUTER SIMULATIO. Sprading squnc optical ZCZ cod Squnc lngth 6 Family siz M 7 6 Zro corrlation zon z um. of th nonzro lmnts w um. of trials 6 Bit rat 56Mbps 3Mbps Chip rat 3,7Mcps Lasr wavlngth λ 83nm APD quantum fficincy η.6 APD gain G APD ffctiv ionization ratio K ff. Bulk lakag currnt I b.na Surfac lakag currnt I s na Modulation xtinction ratio M Rcivr nois tmpratur T r,k Rcivr load rsistor R L,3 Ω Background nois P b -5 dbm Scintillation logarithm varianc σs. { σ m = G F T c λ s w + w m + I b M + I st c + σ th, 3 λ s = ηp w hf, 33 P w = w P bit, 3 G F = K ff G + K ff, 35 G σ th = k BT r T c R L, 36 f = c λ, 37 w = { z+ z+ ; z = n, ; z =, 38 whr µ and σ m ar th avrag and varianc of th corrlation output, m is th numbr of usrs, G is th APD gain, T c is th chip duration, is th squnc lngth, M is th modulation xtinction ratio, λ s is th avrag numbr of absorbd photons ovr T c, w is th numbr of th nonzro lmnts in ach squnc, F is th xcss nois factor, I b is th bulk lakag currnt, I s is th surfac lakag currnt, is th lmntary lctric charg, σth is th varianc of thrmal nois, η is th APD quantum fficincy, P w is th rcivd lasr powr pr chip without scintillation, P bit is th avrag rcivd lasr powr pr bit without scintillation, P b is th background nois pr chip duration T c, h is Planck s constant, f is th optical frquncy, K ff is th APD ffctiv ionization ratio, k B is Boltzmann constant, T r is th rcivr nois tmpratur, R L is th rcivr load rsistor, c is vlocity of light, and λ is th lasr wavlngth. ot that th background nois isn t considrd ovr th optical fibr. Figurs 3 and show BER prformanc of optical ZCZ- CDMA systm with z = and by th lctrical procssing

5 ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, 3 Transmittr d Cod Gnrator â, â, â,d d Cod Gnrator â, â, â,d Optical fibr or spac APD A/D channl Rcivr r i R Elctrical corrlator Data d m Cod Gnrator â m, â m, â m,dm a â, â, Fig.. Optical ZCZ-CDMA systm by th lctrical procssing. Transmittr d Cod Gnrator â, â, â,d Rcivr d Cod Gnrator â, â, â,d Optical fibr or spac channl ˆR r i Optical corrlator APD A/D Splittr + R Optical - APD A/D corrlator ˆR Data d m Cod Gnrator â m, â m, â m,dm â, â, Fig.. Optical ZCZ-CDMA systm by th optical procssing. ovr th optical fibr, rspctivly. Similarly, th thortical formula of BER charactristics of th optical ZCZ-CDMA systm by th optical procssing ovr th optical fibr is givn by p BER = rfc µ, 39 σ m M µ = wgt c λ s M σ m = G F T c { + I st c λ s w + w M = µ, m + I b + σ th. Figurs 5 and 6 show BER prformanc of optical ZCZ- CDMA systm with z = and by th optical procssing ovr th optical fibr, rspctivly. From Figs. 3,, 5 and 6, th optical ZCZ-CDMA systm by th lctrical and optical procssing ovr th optical fibr can t rmov compltly co-channl intrfrnc, and th BER prformanc of this systm by th lctrical procssing ovr th optical fibr go down compard to that by th optical procssing. B. BER prformanc in optical spac transmission Th thortical formula of BER charactristics of th optical ZCZ-CDMA systm by th lctrical procssing ovr th

6 ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, Avrag rcivd lasr powr pr a bit Pbit [dbm] Fig. 3. BER prformanc of optical ZCZ-CDMA systm with z = by th lctrical procssing ovr th optical fibr Avrag rcivd lasr powr pr a bit Pbit [dbm] Fig. 5. BER prformanc of optical ZCZ-CDMA systm with z = by th optical procssing ovr th optical fibr Avrag rcivd lasr powr pr a bit Pbit [dbm] -3 Fig.. BER prformanc of optical ZCZ-CDMA systm with z = by th lctrical procssing ovr th optical fibr Avrag rcivd lasr powr pr a bit Pbit [dbm] -3 Fig. 6. BER prformanc of optical ZCZ-CDMA systm with z = by th optical procssing ovr th optical fibr. optical spac is givn by P BER = pa pa pa m µa rfc da σ A, A,, A m da da m = pa pa µa rfc da da, σ A, A m A = A, 3 pa = = { ln A + σ s xp πσ s A σ s, pa = pa pa m, 5 M µa = wgt c λ s A, 6 M 3 { σ A, A = G F T c λ s w + w A + A +λ b + I b M + I st c + σ th, 7 whr pa is th probability dnsity function of th scintillation A for th m usr, σ s is th scintillation logarithm varianc, µa and σ A, A ar th avrag and varianc of th corrlation output, rspctivly and dnots th convolution as pa pa = pa pa a. 8 a = Figurs 7 and 8 show BER prformanc of optical ZCZ- CDMA systm with z = and by th lctrical procssing ovr th optical spac, rspctivly. Similarly, th thortical formula of BER charactristics of th optical ZCZ-CDMA systm by th optical procssing ovr

7 ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, Avrag rcivd lasr powr pr a bit without scintillation Pbit [dbm] Fig. 7. BER prformanc of optical ZCZ-CDMA systm with z = by th lctrical procssing ovr th optical spac. ovr th optical spac, rspctivly Avrag rcivd lasr powr pr a bit without scintillation Pbit [dbm] Fig. 9. BER prformanc of optical ZCZ-CDMA systm with z = by th optical procssing ovr th optical spac Avrag rcivd lasr powr pr a bit without scintillation Pbit [dbm] Fig. 8. BER prformanc of optical ZCZ-CDMA systm with z = by th lctrical procssing ovr th optical spac Avrag rcivd lasr powr pr a bit without scintillation Pbit [dbm]. th optical spac is givn by P BER = pa pa pa m µa rfc da σ A, A,, A m da da m = pa pa µa rfc da da, 9 σ A, A M µa = wgt c λ s A = µa, 5 M { σ A, A = G F T c λ s w + w A + A +λ b + I b M + I st c + σ th. 5 Figurs 9 and show BER prformanc of optical ZCZ- CDMA systm with z = and by th optical procssing Fig.. BER prformanc of optical ZCZ-CDMA systm with z = by th optical procssing ovr th optical spac. From Figs. 7, 8, 9 and, th optical ZCZ-CDMA systm by th lctrical and optical procssing ovr th optical spac can t rmov compltly co-channl intrfrnc, and th BER prformanc of this systm by th lctrical procssing ovr th optical spac go down compard to that by th optical procssing. From Figs. 3,, 5, 6, 7, 8, 9 and, th BER prformanc of this systm ovr th optical spac go down compard to that ovr th optical fibr. V. COCLUSIOS In this papr, w analyz th BER prformanc of optical ZCZ-CDMA systm with zro-corrlation zon n or by th lctrical and optical procssing ovr th optical fibr and spac with considring th ffcts of th scintillation, APD nois, thrmal nois and co-channl intrfrnc by computr and thortical formula. As a rsult, th BER prformanc of this systm ovr th optical spac go down compard to that ovr th optical fibr, and th BER prformanc of this systm by th lctrical procssing go down compard to that by th optical procssing.

8 ITERATIOAL JOURAL OF COMPUTERS AD COMMUICATIOS Issu, Volum 7, 3 8 Th optical ZCZ-CDMA systm by th lctrical and optical procssing can t rmov compltly co-channl intrfrnc. ACKOWLEDGMET This rsarch was supportd by th Ministry of Education,Cultur, Sports, Scinc and Tchnology MEXT, Grantin-Aids for Young Scintists B769 and challnging Exploratory Rsarch REFERECES [] J. G. Zhang and G. Picchi, Tunabl prim-cod ncodr/dcodr for all-optical CDMA applications, IEE Elctron. Ltt., vol. 9, no. 3, 993, pp.. [] J. A. Salhi, A. M. Winr and J. P. Hritag, Cohrnt ultrashort light puls cod-division multipl accss communication systms, IEEE J. Lightwav Tchnol., vol. 8, no. 3, 99, pp [3] H. Fathallah, L. A. Rusch and S. LaRochll, Passiv optical fast frquncy-hop CDMA communications systm, IEEE J. Lightwav Tchnol., vol. 7, no. 3, 999, pp [] T. Otsuki, Prformanc analysis of atmosphric optical PPM CDMA systms, IEEE J. Lightwav Tchnol., vol., no., 99, pp [5] Y. Kozawa and H. Habuchi, Thortical analysis of optical wirlss CDMA with modifid psudo orthogonal M-squnc sts, Proc. of IEEE Global Communications Confrnc, Exhibition and Industry Forum Co-locatd with WTCGLOBECOM9, 9. [6] Y. Kozawa and H. Habuchi, A comparison of wirlss optical CDMA systms using chip-lvl dtction, IEICE Trans. Fundam., vol. E93-A, no.,, pp [7] A. T. Pham and H. Yashima, Prformanc Analysis of Rd-Solomon Codd Spctral Amplitud Encoding OCDMA Systm, WSEAS Trans. on Elctronics, Issu, vol.,, pp [8] Y. Mizuno and H. Yashima, Optical CDMA systms using xtndd chaotic binary cods, J. Signal Procssing, vol., no.,, pp [9] P. Z. Fan and M. Darnll, Squnc dsign for communications applications, Rsarch Studis Prss, 996. [] S. Matsufui, T. Matsumoto, Y. Tanada and. Kuroyanagi, ZCZ cods for ASK-CDMA systm, IEICE Trans. Fundam., vol. E89-A, no. 9, 6, pp [] T. Matsumoto, M. Inou, H. Torii and S. Matsufui, Study on BER Prformanc of Atmosphric Optical CDMA Systm Using Optical ZCZ Cod, Proc. of th RISP Intrnational Workshop on onlinar Circuits, Communications and Signal Procssing,, pp [] T. Matsumoto, H. Torii and S. Matsufui, Thortical Analysis of BER Prformanc of Optical ZCZ-CDMA Systm With Smallst Zro Corrlation Zon Using Optical Corrlator, Proc. of th IEEE Intrnational Symposium on Intllignt Signal Procssing and Communication Systms,, pp [3] T. Matsumoto, H. Torii and S. Matsufui, Comparison of Optical ZCZ-CDMA Systm with Zro Corrlation Zon n by Elctrical and Optical Procssing, Proc. of th 3rd Europan Confrnc of Communications, pp [] T. Matsumoto and S. Matsufui, Optical ZCZ cod gnrators using Sylvstr-typ Hadamard matrix, Intrnational J. of Communications, Issu, vol.,, pp. 9. [5] T. Matsumoto, S. Tsukiashi, S. Matsufui and Y. Tanada, Th bank of matchd filtrs for an optical ZCZ cod using a Sylvstr typ Hadamard matrix, IEICE Trans. Fundam., vol. E89-A, no. 9, 6, pp [6] T. Matsumoto and S. Matsufui, Compact matchd filtr banks of optical ZCZ cods using fast algorithm for M-squnc typ Hadamard matrix, J. Signal Procssing, vol., no. 6,, pp Takahiro Matsumoto rcivd his B. Eng. and M. Eng. dgrs in Information and Computr Scinc from Kagoshima Univrsity, Japan, in 996 and 998, rspctivly, and his Ph. D. dgr in Enginring from Yamaguchi Univrsity, Japan, in 7. H was a Rsarch Associat from 998 to 7 and an Assistant Profssor from 7 to at Yamaguchi Univrsity, Japan. Sinc, h has bn an Associat Profssor of th Univrsity Evaluation Dpartmnt at Yamaguchi Univrsity. From to, h was a visiting rsarchr at th Univrsity of Mlbourn, Australia. His currnt rsarch intrsts includ sprad spctrum systms and thir applications. H rcivd th Bst Papr Award in th th WSEAS Intnational Confrnc on Applid Informatics and Communications in. H is a mmbr of IEEE and IEICE. Hidyuki Torii rcivd th B. Eng., M. Eng., and Ph. D. dgrs from th Univrsity of Tsukuba, Tsukuba, Japan in 995, 997, and rspctivly. In, h oind th Dpartmnt of twork Enginring, Kanagawa Institut of Tchnology as a Rsarch Associat. H is currntly an Associat Profssor in th Dpartmnt of Information twork and Communication at th sam univrsity. His rsarch intrsts includ sprading squncs, CDMA systms, and mobil communication systms. H is a mmbr of IEEE and IEICE. Shinya Matsufui graduatd from th Dpartmnt of Elctronic Enginring at Fukuoka Univrsity in 977. H rcivd th Dr. Eng. in Computr Scinc and Communication Enginring from Kyushu Univrsity, Fukuoka, Japan in 993. From 977 to 98, h was a tchnical official at Saga Univrsity, Saga, Japan. From 98 to, h was a rsarch associat in th Dpartmnt of Information Scinc at Saga Univrsity. From to, h was an associat profssor of th Dpartmnt of Computr Scinc and Systms Enginring at Yamaguchi Univrsity. Sinc, h has bn a profssor of th Graduat School of Scinc and Enginring at Yamaguchi Univrsity. His currnt rsarch intrsts includ squnc dsign and sprad spctrum systms. H rcivd th Excllnt Papr Award in IET Intrnational Communication Confrnc on Wirlss Mobil and Computing, and th Bst Papr Award in th th WSEAS Intnational Confrnc on Applid Informatics and Communications in 9 and, rspctivly. H is a mmbr of IEEE, IEICE and IEEJ. 5

Zero Vectors Combinatorial Code Family for Spectral Amplitude Coding (SAC-OCDMA)

Zero Vectors Combinatorial Code Family for Spectral Amplitude Coding (SAC-OCDMA) 0 IJCSNS Intrnational Journal of Computr Scinc and Ntwork Scurity, VOL.8 No.3, March 008 Zro Vctors Combinatorial Cod Family for Spctral Amplitud Coding (SAC-OCDMA) Hassan Yousif Ahmd, Ibrahima Fay, and

More information

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is

Procdings of IC-IDC0 ( and (, ( ( and (, and (f ( and (, rspctivly. If two input signals ar compltly qual, phas spctra of two signals ar qual. That is Procdings of IC-IDC0 EFFECTS OF STOCHASTIC PHASE SPECTRUM DIFFERECES O PHASE-OLY CORRELATIO FUCTIOS PART I: STATISTICALLY COSTAT PHASE SPECTRUM DIFFERECES FOR FREQUECY IDICES Shunsu Yamai, Jun Odagiri,

More information

Code Cross-Correlation Effects on the Performance of Optical CDMA Systems in the Presence of Receiver Noises

Code Cross-Correlation Effects on the Performance of Optical CDMA Systems in the Presence of Receiver Noises 0 8th Intrnational Confrnc on Tlcommunications Cod Cross-Corrlation Effcts on th Prformanc of Optical CDMA Systms in th Prsnc of Rcivr Noiss S. M. Zabihi-Maddah M. Molavi Kakhki Faculty of Enginring, Frdowsi

More information

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes Procdings of th 9th WSEAS Intrnational Confrnc on APPLICATIONS of COMPUTER ENGINEERING A Sub-Optimal Log-Domain Dcoding Algorithm for Non-Binary LDPC Cods CHIRAG DADLANI and RANJAN BOSE Dpartmnt of Elctrical

More information

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac.

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac. Lctur 2: Discrt-Tim Signals & Systms Rza Mohammadkhani, Digital Signal Procssing, 2015 Univrsity of Kurdistan ng.uok.ac.ir/mohammadkhani 1 Signal Dfinition and Exampls 2 Signal: any physical quantity that

More information

PHASE-ONLY CORRELATION IN FINGERPRINT DATABASE REGISTRATION AND MATCHING

PHASE-ONLY CORRELATION IN FINGERPRINT DATABASE REGISTRATION AND MATCHING Anall Univrsităţii d Vst din Timişoara Vol. LII, 2008 Sria Fizică PHASE-OLY CORRELATIO I FIGERPRIT DATABASE REGISTRATIO AD ATCHIG Alin C. Tusda, 2 Gianina Gabor Univrsity of Orada, Environmntal Faculty,

More information

2. Background Material

2. Background Material S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds

More information

Communication Technologies

Communication Technologies Communication Tchnologis. Principls of Digital Transmission. Structur of Data Transmission.2 Spctrum of a Data Signal 2. Digital Modulation 2. Linar Modulation Mthods 2.2 Nonlinar Modulations (CPM-Signals)

More information

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient

Full Waveform Inversion Using an Energy-Based Objective Function with Efficient Calculation of the Gradient Full Wavform Invrsion Using an Enrgy-Basd Objctiv Function with Efficint Calculation of th Gradint Itm yp Confrnc Papr Authors Choi, Yun Sok; Alkhalifah, ariq Ali Citation Choi Y, Alkhalifah (217) Full

More information

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions. Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind

More information

SER/BER in a Fading Channel

SER/BER in a Fading Channel SER/BER in a Fading Channl Major points for a fading channl: * SNR is a R.V. or R.P. * SER(BER) dpnds on th SNR conditional SER(BER). * Two prformanc masurs: outag probability and avrag SER(BER). * Ovrall,

More information

Phase Rotation for the 80 MHz ac Mixed Mode Packet

Phase Rotation for the 80 MHz ac Mixed Mode Packet Phas Rotation for th 80 MHz 802.11ac Mixd Mod Packt Dat: 2010-07-12 Authors: Nam Affiliations Addrss Phon mail Lonardo Lanant Jr. Kyushu Inst. of Tchnology Kawazu 680-, Iizuka, JAPAN Yuhi Nagao Kyushu

More information

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator

Calculation of electromotive force induced by the slot harmonics and parameters of the linear generator Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,

More information

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN Intrnational Journal of Scintific & Enginring Rsarch, Volum 6, Issu 7, July-25 64 ISSN 2229-558 HARATERISTIS OF EDGE UTSET MATRIX OF PETERSON GRAPH WITH ALGEBRAI GRAPH THEORY Dr. G. Nirmala M. Murugan

More information

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology Bluchr Mchanical Enginring Procdings May 2014, vol. 1, num. 1 www.procdings.bluchr.com.br/vnto/10wccm TOPOLOGY DESIG OF STRUCTURE LOADED BY EARTHQUAKE P. Rosko 1 1 Cntr of Mchanics and Structural Dynamics,

More information

Homotopy perturbation technique

Homotopy perturbation technique Comput. Mthods Appl. Mch. Engrg. 178 (1999) 257±262 www.lsvir.com/locat/cma Homotopy prturbation tchniqu Ji-Huan H 1 Shanghai Univrsity, Shanghai Institut of Applid Mathmatics and Mchanics, Shanghai 272,

More information

Koch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna

Koch Fractal Boundary Single feed Circularly Polarized Microstrip Antenna 1 Journal of Microwavs, Optolctronics and Elctromagntic Applications, Vol. 6, No. 2, Dcmbr 2007 406 Koch Fractal Boundary Singl fd Circularly Polarizd Microstrip Antnna P. Nagswara Rao and N. V. S.N Sarma

More information

The pn junction: 2 Current vs Voltage (IV) characteristics

The pn junction: 2 Current vs Voltage (IV) characteristics Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n

More information

10. The Discrete-Time Fourier Transform (DTFT)

10. The Discrete-Time Fourier Transform (DTFT) Th Discrt-Tim Fourir Transform (DTFT Dfinition of th discrt-tim Fourir transform Th Fourir rprsntation of signals plays an important rol in both continuous and discrt signal procssing In this sction w

More information

Image Filtering: Noise Removal, Sharpening, Deblurring. Yao Wang Polytechnic University, Brooklyn, NY11201

Image Filtering: Noise Removal, Sharpening, Deblurring. Yao Wang Polytechnic University, Brooklyn, NY11201 Imag Filtring: Nois Rmoval, Sharpning, Dblurring Yao Wang Polytchnic Univrsity, Brooklyn, NY http://wb.poly.du/~yao Outlin Nois rmoval by avraging iltr Nois rmoval by mdian iltr Sharpning Edg nhancmnt

More information

Quasi-Classical States of the Simple Harmonic Oscillator

Quasi-Classical States of the Simple Harmonic Oscillator Quasi-Classical Stats of th Simpl Harmonic Oscillator (Draft Vrsion) Introduction: Why Look for Eignstats of th Annihilation Oprator? Excpt for th ground stat, th corrspondnc btwn th quantum nrgy ignstats

More information

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a

Rotor Stationary Control Analysis Based on Coupling KdV Equation Finite Steady Analysis Liu Dalong1,a, Xu Lijuan2,a 204 Intrnational Confrnc on Computr Scinc and Elctronic Tchnology (ICCSET 204) Rotor Stationary Control Analysis Basd on Coupling KdV Equation Finit Stady Analysis Liu Dalong,a, Xu Lijuan2,a Dpartmnt of

More information

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012 Th van dr Waals intraction D. E. Sopr 2 Univrsity of Orgon 20 pril 202 Th van dr Waals intraction is discussd in Chaptr 5 of J. J. Sakurai, Modrn Quantum Mchanics. Hr I tak a look at it in a littl mor

More information

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS Slid DIGITAL SIGAL PROCESSIG UIT I DISCRETE TIME SIGALS AD SYSTEM Slid Rviw of discrt-tim signals & systms Signal:- A signal is dfind as any physical quantity that varis with tim, spac or any othr indpndnt

More information

Introduction to the Fourier transform. Computer Vision & Digital Image Processing. The Fourier transform (continued) The Fourier transform (continued)

Introduction to the Fourier transform. Computer Vision & Digital Image Processing. The Fourier transform (continued) The Fourier transform (continued) Introduction to th Fourir transform Computr Vision & Digital Imag Procssing Fourir Transform Lt f(x) b a continuous function of a ral variabl x Th Fourir transform of f(x), dnotd by I {f(x)} is givn by:

More information

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013 18.782 Introduction to Arithmtic Gomtry Fall 2013 Lctur #20 11/14/2013 20.1 Dgr thorm for morphisms of curvs Lt us rstat th thorm givn at th nd of th last lctur, which w will now prov. Thorm 20.1. Lt φ:

More information

Apparent Power and Power Factor Measurement by Using FPGA-based Chip Considering Nonsinusoidal and Unbalanced Conditions

Apparent Power and Power Factor Measurement by Using FPGA-based Chip Considering Nonsinusoidal and Unbalanced Conditions Procdings of t 8t WE Intrnational Confrnc on Instrumntation, Masurmnt, Circuits and ystms pparnt Powr and Powr Factor Masurmnt by Using FPG-basd Cip Considring Nonsinusoidal and Unbalancd Conditions HU-CHEN

More information

EEO 401 Digital Signal Processing Prof. Mark Fowler

EEO 401 Digital Signal Processing Prof. Mark Fowler EEO 401 Digital Signal Procssing Prof. Mark Fowlr Dtails of th ot St #19 Rading Assignmnt: Sct. 7.1.2, 7.1.3, & 7.2 of Proakis & Manolakis Dfinition of th So Givn signal data points x[n] for n = 0,, -1

More information

VII. Quantum Entanglement

VII. Quantum Entanglement VII. Quantum Entanglmnt Quantum ntanglmnt is a uniqu stat of quantum suprposition. It has bn studid mainly from a scintific intrst as an vidnc of quantum mchanics. Rcntly, it is also bing studid as a basic

More information

Sliding Mode Flow Rate Observer Design

Sliding Mode Flow Rate Observer Design Sliding Mod Flow Rat Obsrvr Dsign Song Liu and Bin Yao School of Mchanical Enginring, Purdu Univrsity, Wst Lafaytt, IN797, USA liu(byao)@purdudu Abstract Dynamic flow rat information is ndd in a lot of

More information

Voltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes

Voltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes Lctur 1. oltag, Currnt, Powr, Sris sistanc, Paralll sistanc, and Diods Whn you start to dal with lctronics thr ar thr main concpts to start with: Nam Symbol Unit oltag volt Currnt ampr Powr W watt oltag

More information

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Construction of asymmetric orthogonal arrays of strength three via a replacement method isid/ms/26/2 Fbruary, 26 http://www.isid.ac.in/ statmath/indx.php?modul=prprint Construction of asymmtric orthogonal arrays of strngth thr via a rplacmnt mthod Tian-fang Zhang, Qiaoling Dng and Alok Dy

More information

Random Process Part 1

Random Process Part 1 Random Procss Part A random procss t (, ζ is a signal or wavform in tim. t : tim ζ : outcom in th sampl spac Each tim w rapat th xprimnt, a nw wavform is gnratd. ( W will adopt t for short. Tim sampls

More information

Problem Set #2 Due: Friday April 20, 2018 at 5 PM.

Problem Set #2 Due: Friday April 20, 2018 at 5 PM. 1 EE102B Spring 2018 Signal Procssing and Linar Systms II Goldsmith Problm St #2 Du: Friday April 20, 2018 at 5 PM. 1. Non-idal sampling and rcovry of idal sampls by discrt-tim filtring 30 pts) Considr

More information

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017

Radiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017 Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.

More information

The failure of the classical mechanics

The failure of the classical mechanics h failur of th classical mchanics W rviw som xprimntal vidncs showing that svral concpts of classical mchanics cannot b applid. - h blac-body radiation. - Atomic and molcular spctra. - h particl-li charactr

More information

Coupled Pendulums. Two normal modes.

Coupled Pendulums. Two normal modes. Tim Dpndnt Two Stat Problm Coupld Pndulums Wak spring Two normal mods. No friction. No air rsistanc. Prfct Spring Start Swinging Som tim latr - swings with full amplitud. stationary M +n L M +m Elctron

More information

Principles of active remote sensing: Lidars. 1. Optical interactions of relevance to lasers. Lecture 22

Principles of active remote sensing: Lidars. 1. Optical interactions of relevance to lasers. Lecture 22 Lctur 22 Principls of activ rmot snsing: Lidars Ojctivs: 1. Optical intractions of rlvanc to lasrs. 2. Gnral principls of lidars. 3. Lidar quation. quird rading: G: 8.4.1, 8.4.2 Additional/advancd rading:.m.

More information

ECE507 - Plasma Physics and Applications

ECE507 - Plasma Physics and Applications ECE507 - Plasma Physics and Applications Lctur 7 Prof. Jorg Rocca and Dr. Frnando Tomasl Dpartmnt of Elctrical and Computr Enginring Collisional and radiativ procsss All particls in a plasma intract with

More information

Human vision is determined based on information theory:

Human vision is determined based on information theory: Human vision is dtrmind basd on information thory: Supplmntary Information Alfonso Dlgado-Bonal,2 and F. Javir Martn Torrs,3 [] Instituto Andaluz d Cincias d la Tirra CSIC-UGR, Avda. d Las Palmras n 4,

More information

On the Hamiltonian of a Multi-Electron Atom

On the Hamiltonian of a Multi-Electron Atom On th Hamiltonian of a Multi-Elctron Atom Austn Gronr Drxl Univrsity Philadlphia, PA Octobr 29, 2010 1 Introduction In this papr, w will xhibit th procss of achiving th Hamiltonian for an lctron gas. Making

More information

A Propagating Wave Packet Group Velocity Dispersion

A Propagating Wave Packet Group Velocity Dispersion Lctur 8 Phys 375 A Propagating Wav Packt Group Vlocity Disprsion Ovrviw and Motivation: In th last lctur w lookd at a localizd solution t) to th 1D fr-particl Schrödingr quation (SE) that corrsponds to

More information

A Control Strategy for Photovoltaic-Solid Polymer Electrolysis System Based on Surface Temperature of PV Panel

A Control Strategy for Photovoltaic-Solid Polymer Electrolysis System Based on Surface Temperature of PV Panel Amrican Journal of Applid Scincs 5 (7): 5-, ISSN 1546-939 Scinc Publications Corrsponding Author: A Control Stratgy for Photovoltaic-Solid Polymr Elctrolysis Systm Basd on Surfac Tmpratur of PV Panl 1

More information

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let It is impossibl to dsign an IIR transfr function with an xact linar-phas It is always possibl to dsign an FIR transfr function with an xact linar-phas rspons W now dvlop th forms of th linarphas FIR transfr

More information

Abstract Interpretation: concrete and abstract semantics

Abstract Interpretation: concrete and abstract semantics Abstract Intrprtation: concrt and abstract smantics Concrt smantics W considr a vry tiny languag that manags arithmtic oprations on intgrs valus. Th (concrt) smantics of th languags cab b dfind by th funzcion

More information

A Zero-IF digitized Despreading Scheme Without PN Code Synchronization Recovery

A Zero-IF digitized Despreading Scheme Without PN Code Synchronization Recovery A Zro-IF digitizd Dsprading Schm Without PN Cod Synchronization Rcovry Hong Guo, Fng Guo Xidian Univ.MCN Group 119#, aiainan Road, Xi an, Shaanxi, P.R.China (zip cod:7171 hguo@mcn.xidian.du.cn ao Duan

More information

Evaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker

Evaluating Reliability Systems by Using Weibull & New Weibull Extension Distributions Mushtak A.K. Shiker Evaluating Rliability Systms by Using Wibull & Nw Wibull Extnsion Distributions Mushtak A.K. Shikr مشتاق عبذ الغني شخير Univrsity of Babylon, Collg of Education (Ibn Hayan), Dpt. of Mathmatics Abstract

More information

(Upside-Down o Direct Rotation) β - Numbers

(Upside-Down o Direct Rotation) β - Numbers Amrican Journal of Mathmatics and Statistics 014, 4(): 58-64 DOI: 10593/jajms0140400 (Upsid-Down o Dirct Rotation) β - Numbrs Ammar Sddiq Mahmood 1, Shukriyah Sabir Ali,* 1 Dpartmnt of Mathmatics, Collg

More information

Application of Vague Soft Sets in students evaluation

Application of Vague Soft Sets in students evaluation Availabl onlin at www.plagiarsarchlibrary.com Advancs in Applid Scinc Rsarch, 0, (6):48-43 ISSN: 0976-860 CODEN (USA): AASRFC Application of Vagu Soft Sts in studnts valuation B. Chtia*and P. K. Das Dpartmnt

More information

Properties of Phase Space Wavefunctions and Eigenvalue Equation of Momentum Dispersion Operator

Properties of Phase Space Wavefunctions and Eigenvalue Equation of Momentum Dispersion Operator Proprtis of Phas Spac Wavfunctions and Eignvalu Equation of Momntum Disprsion Oprator Ravo Tokiniaina Ranaivoson 1, Raolina Andriambololona 2, Hanitriarivo Rakotoson 3 raolinasp@yahoo.fr 1 ;jacqulinraolina@hotmail.com

More information

ECE 344 Microwave Fundamentals

ECE 344 Microwave Fundamentals ECE 44 Microwav Fundamntals Lctur 08: Powr Dividrs and Couplrs Part Prpard By Dr. hrif Hkal 4/0/08 Microwav Dvics 4/0/08 Microwav Dvics 4/0/08 Powr Dividrs and Couplrs Powr dividrs, combinrs and dirctional

More information

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic

More information

Title: Vibrational structure of electronic transition

Title: Vibrational structure of electronic transition Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum

More information

by wavelength modulation of a distributed-feedback laser

by wavelength modulation of a distributed-feedback laser Prformanc analysis of a timdivision-multiplxd fibr-optic gas-snsor array by wavlngth modulation of a distributd-fdback lasr Wi Jin Th rsults of an invstigation of th prformanc of a tim-division-addrssd

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME Introduction to Finit Elmnt Analysis Chaptr 5 Two-Dimnsional Formulation Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

Radar Signal Demixing via Convex Optimization

Radar Signal Demixing via Convex Optimization Radar Signal Dmixing via Convx Optimization Gongguo Tang Dpartmnt of Elctrical Enginring Colorado School of Mins DSP 2017 Joint work with Youy Xi, Shuang Li, and Michal B. Wakin (Colorado School of Mins)

More information

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation.

Fourier Transforms and the Wave Equation. Key Mathematics: More Fourier transform theory, especially as applied to solving the wave equation. Lur 7 Fourir Transforms and th Wav Euation Ovrviw and Motivation: W first discuss a fw faturs of th Fourir transform (FT), and thn w solv th initial-valu problm for th wav uation using th Fourir transform

More information

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim.

COHORT MBA. Exponential function. MATH review (part2) by Lucian Mitroiu. The LOG and EXP functions. Properties: e e. lim. MTH rviw part b Lucian Mitroiu Th LOG and EXP functions Th ponntial function p : R, dfind as Proprtis: lim > lim p Eponntial function Y 8 6 - -8-6 - - X Th natural logarithm function ln in US- log: function

More information

The Control of Electromagnetic Filter by Using FPGA Based PI Type Fuzzy Controller

The Control of Electromagnetic Filter by Using FPGA Based PI Type Fuzzy Controller Th Control of Elctromagntic Filtr by Using FPGA Basd PI Typ Fuzzy Controllr Ilkr Ali OZKAN a, Ismail SARITAS b, Saadtdin HERDEM b a Dpartmnt of Computr Enginring, b Dpartmnt of Elctrical and Elctronics

More information

Tishreen University Journal for Research and Scientific Studies - Engineering Sciences Series Vol. ( ) No. ( ) Fractal Geometry.

Tishreen University Journal for Research and Scientific Studies - Engineering Sciences Series Vol. ( ) No. ( ) Fractal Geometry. Tishrn Univrsity Journal for Rsarch and Scintific Studis - nginring Scincs Sris Vol. ( ) o. ( ) Fractal Gomtry Auto-similarity a.salh@fr.fr ١١٣ Tishrn Univrsity Journal for Rsarch and Scintific Studis

More information

Discrete Hilbert Transform. Numeric Algorithms

Discrete Hilbert Transform. Numeric Algorithms Volum 49, umbr 4, 8 485 Discrt Hilbrt Transform. umric Algorithms Ghorgh TODORA, Rodica HOLOEC and Ciprian IAKAB Abstract - Th Hilbrt and Fourir transforms ar tools usd for signal analysis in th tim/frquncy

More information

Contemporary, atomic, nuclear, and particle physics

Contemporary, atomic, nuclear, and particle physics Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is

More information

Dynamic response of a finite length euler-bernoulli beam on linear and nonlinear viscoelastic foundations to a concentrated moving force

Dynamic response of a finite length euler-bernoulli beam on linear and nonlinear viscoelastic foundations to a concentrated moving force Journal of Mchanical Scinc and Tchnology 2 (1) (21) 1957~1961 www.springrlink.com/contnt/1738-9x DOI 1.17/s1226-1-7-x Dynamic rspons of a finit lngth ulr-brnoulli bam on linar and nonlinar viscolastic

More information

Types of Transfer Functions. Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters

Types of Transfer Functions. Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters Typs of Transfr Typs of Transfr x[n] X( LTI h[n] H( y[n] Y( y [ n] h[ k] x[ n k] k Y ( H ( X ( Th tim-domain classification of an LTI digital transfr function is basd on th lngth of its impuls rspons h[n]:

More information

THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION

THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION 5th Europan Signal Procssing Confrnc (EUSIPCO 007), Poznan, Poland, Sptmbr 3-7, 007, copyright by EURASIP THE IMPACT OF A PRIORI INFORMATION ON THE MAP EQUALIZER PERFORMANCE WITH M-PSK MODULATION Chaabouni

More information

Why is a E&M nature of light not sufficient to explain experiments?

Why is a E&M nature of light not sufficient to explain experiments? 1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt

More information

5.80 Small-Molecule Spectroscopy and Dynamics

5.80 Small-Molecule Spectroscopy and Dynamics MIT OpnCoursWar http://ocw.mit.du 5.80 Small-Molcul Spctroscopy and Dynamics Fall 008 For information about citing ths matrials or our Trms of Us, visit: http://ocw.mit.du/trms. Lctur # 3 Supplmnt Contnts

More information

THE P-PERSISTENT CSMA WITH THE FUNCTION OF MONITORING BASED ON TIME DIVISION MECHA- NISM

THE P-PERSISTENT CSMA WITH THE FUNCTION OF MONITORING BASED ON TIME DIVISION MECHA- NISM ISSN:3-56 Intrnational Journal of Innovativ Rsarch in Tchnology & Scinc(IJIRTS) THE P-PERSISTENT CSMA WITH THE FUNCTION OF MONITORING BASED ON TIME DIVISION MECHA- NISM Yifan Zhao, Yunnan Univrsity, Kunming,

More information

STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS

STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS Journal of Optolctronics and Advancd Matrials Vol. 6 No. March 4 p. 63-69 STATISTICAL PROPERTIES ANALYSIS OF Er 3+ -DOPED Ti:LiNbO 3 M -MODE STRAIGHT WAVEGUIDE AMPLIFIERS N. N. Puscas * Physics Dpartmnt

More information

1 2 precise electro-optic switch in periodically poled lithium niobate

1 2 precise electro-optic switch in periodically poled lithium niobate 1 2 prcis lctro-optic switch in priodically pold lithium niobat Juan Huo, Kun Liu, Xianfng Chn* Dpartmnt of Physics; Th Stat Ky Laboratory on Fibr Optic Local Ara Communication Ntworks and Advancd Optical

More information

Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters. Ideal Filters

Types of Transfer Functions. Types of Transfer Functions. Ideal Filters. Ideal Filters. Ideal Filters Typs of Transfr Typs of Transfr Th tim-domain classification of an LTI digital transfr function squnc is basd on th lngth of its impuls rspons: - Finit impuls rspons (FIR) transfr function - Infinit impuls

More information

Effects of Electron Model on Three-Grid Ion Engine Analyses

Effects of Electron Model on Three-Grid Ion Engine Analyses Effcts of Elctron Modl on Thr-Grid Ion Engin Analyss IEPC-2011-205 Prsntd at th 32nd Intrnational Elctric Propulsion Confrnc, Wisbadn Grmany Takshi Miyasaka 1 and Katsuo Asato 2 Gifu Univrsity, Gifu, 501-1193,

More information

Two Products Manufacturer s Production Decisions with Carbon Constraint

Two Products Manufacturer s Production Decisions with Carbon Constraint Managmnt Scinc and Enginring Vol 7 No 3 pp 3-34 DOI:3968/jms9335X374 ISSN 93-34 [Print] ISSN 93-35X [Onlin] wwwcscanadant wwwcscanadaorg Two Products Manufacturr s Production Dcisions with Carbon Constraint

More information

1 Isoparametric Concept

1 Isoparametric Concept UNIVERSITY OF CALIFORNIA BERKELEY Dpartmnt of Civil Enginring Spring 06 Structural Enginring, Mchanics and Matrials Profssor: S. Govindj Nots on D isoparamtric lmnts Isoparamtric Concpt Th isoparamtric

More information

MCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems

MCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems MCE503: Modling and Simulation o Mchatronic Systms Discussion on Bond Graph Sign Convntions or Elctrical Systms Hanz ichtr, PhD Clvland Stat Univrsity, Dpt o Mchanical Enginring 1 Basic Assumption In a

More information

Search sequence databases 3 10/25/2016

Search sequence databases 3 10/25/2016 Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an

More information

Outline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing-

Outline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing- Outlin Advancd Multimdia Signal Procssing #5:Spch Signal Procssing -Procssing- Intllignt Elctronic Systms Group Dpt. of Elctronic Enginring, UEC Basis of Spch Procssing Nois Rmoval Spctral Subtraction

More information

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance

Design Guidelines for Quartz Crystal Oscillators. R 1 Motional Resistance L 1 Motional Inductance C 1 Motional Capacitance C 0 Shunt Capacitance TECHNICAL NTE 30 Dsign Guidlins for Quartz Crystal scillators Introduction A CMS Pirc oscillator circuit is wll known and is widly usd for its xcllnt frquncy stability and th wid rang of frquncis ovr which

More information

Module 8 Non equilibrium Thermodynamics

Module 8 Non equilibrium Thermodynamics Modul 8 Non quilibrium hrmodynamics ctur 8.1 Basic Postulats NON-EQUIIRIBIUM HERMODYNAMICS Stady Stat procsss. (Stationary) Concpt of ocal thrmodynamic qlbm Extnsiv proprty Hat conducting bar dfin proprtis

More information

Deepak Rajput

Deepak Rajput Q Prov: (a than an infinit point lattic is only capabl of showing,, 4, or 6-fold typ rotational symmtry; (b th Wiss zon law, i.. if [uvw] is a zon axis and (hkl is a fac in th zon, thn hu + kv + lw ; (c

More information

u 3 = u 3 (x 1, x 2, x 3 )

u 3 = u 3 (x 1, x 2, x 3 ) Lctur 23: Curvilinar Coordinats (RHB 8.0 It is oftn convnint to work with variabls othr than th Cartsian coordinats x i ( = x, y, z. For xampl in Lctur 5 w mt sphrical polar and cylindrical polar coordinats.

More information

SIMPLE ONE-DIMENSIONAL CALCULATION OF HALL THRUSTER FLOWFIELDS

SIMPLE ONE-DIMENSIONAL CALCULATION OF HALL THRUSTER FLOWFIELDS SIMPLE ONE-DIMENSIONAL CALCULATION OF HALL THRUSTER FLOWFIELDS Hirokazu Tahara, Takashi Fujioka, Atsushi Shirasakiand Takao Yoshikawa Graduat School of Enginring Scinc, Osaka Univrsity 1-3, Machikanyama,

More information

Unquantized and Uncoded Channel State Information Feedback on Wireless Channels

Unquantized and Uncoded Channel State Information Feedback on Wireless Channels Unquantizd and Uncodd Channl Stat Information Fdback on Wirlss Channls Dragan Samardzija Bll Labs, Lucnt Tchnologis 791 Holmdl-Kyport Road, Holmdl, J 07733, USA Email: dragan@bll-labscom arayan Mandayam

More information

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly

More information

CIRCULAR GRATING ECCENTRIC TESTING AND ERROR COMPENSATION FOR ROBOT JOINT USING DOUBLE READING HEAD

CIRCULAR GRATING ECCENTRIC TESTING AND ERROR COMPENSATION FOR ROBOT JOINT USING DOUBLE READING HEAD 10 th April 013. Vol. 50 No.1 005-013 JATIT & LLS. All rights rsrvd. ISSN: 199-8645 www.jatit.org E-ISSN: 1817-3195 CIRCULAR GRATING ECCENTRIC TESTING AND ERROR COMPENSATION FOR ROBOT JOINT USING DOUBLE

More information

10. Limits involving infinity

10. Limits involving infinity . Limits involving infinity It is known from th it ruls for fundamntal arithmtic oprations (+,-,, ) that if two functions hav finit its at a (finit or infinit) point, that is, thy ar convrgnt, th it of

More information

ANALYSIS IN THE FREQUENCY DOMAIN

ANALYSIS IN THE FREQUENCY DOMAIN ANALYSIS IN THE FREQUENCY DOMAIN SPECTRAL DENSITY Dfinition Th spctral dnsit of a S.S.P. t also calld th spctrum of t is dfind as: + { γ }. jτ γ τ F τ τ In othr words, of th covarianc function. is dfind

More information

Finite Element Model of a Ferroelectric

Finite Element Model of a Ferroelectric Excrpt from th Procdings of th COMSOL Confrnc 200 Paris Finit Elmnt Modl of a Frrolctric A. Lópz, A. D Andrés and P. Ramos * GRIFO. Dpartamnto d Elctrónica, Univrsidad d Alcalá. Alcalá d Hnars. Madrid,

More information

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS

More information

Chapter 6. The Discrete Fourier Transform and The Fast Fourier Transform

Chapter 6. The Discrete Fourier Transform and The Fast Fourier Transform Pusan ational Univrsity Chaptr 6. Th Discrt Fourir Transform and Th Fast Fourir Transform 6. Introduction Frquncy rsponss of discrt linar tim invariant systms ar rprsntd by Fourir transform or z-transforms.

More information

Topology Optimization of Suction Muffler for Noise Attenuation

Topology Optimization of Suction Muffler for Noise Attenuation Purdu Univrsity Purdu -Pubs Intrnational Comprssor Enginring Confrnc School of Mchanical Enginring 2012 Topology Optimization of Suction Mufflr for Nois Attnuation Jin Woo L jinwool@ajou.ac.kr Dong Wook

More information

Davisson Germer experiment

Davisson Germer experiment Announcmnts: Davisson Grmr xprimnt Homwork st 5 is today. Homwork st 6 will b postd latr today. Mad a good guss about th Nobl Priz for 2013 Clinton Davisson and Lstr Grmr. Davisson won Nobl Priz in 1937.

More information

E hf. hf c. 2 2 h 2 2 m v f ' f 2f ' f cos c

E hf. hf c. 2 2 h 2 2 m v f ' f 2f ' f cos c EXPERIMENT 9: COMPTON EFFECT Rlatd Topics Intractions of photons with lctrons, consrvation of momntum and nrgy, inlastic and lastic scattring, intraction cross sction, Compton wavlngth. Principl Whn photons

More information

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007 Optics and Non-Linar Optics I - 007 Non-linar Optics Tutorial Sht Novmbr 007 1. An altrnativ xponntial notion somtims usd in NLO is to writ Acos (") # 1 ( Ai" + A * $i" ). By using this notation and substituting

More information

Basic Polyhedral theory

Basic Polyhedral theory Basic Polyhdral thory Th st P = { A b} is calld a polyhdron. Lmma 1. Eithr th systm A = b, b 0, 0 has a solution or thr is a vctorπ such that π A 0, πb < 0 Thr cass, if solution in top row dos not ist

More information

Introduction to Condensed Matter Physics

Introduction to Condensed Matter Physics Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at

More information

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis

Middle East Technical University Department of Mechanical Engineering ME 413 Introduction to Finite Element Analysis Middl East Tchnical Univrsity Dpartmnt of Mchanical Enginring ME 43 Introduction to Finit Elmnt Analysis Chaptr 3 Computr Implmntation of D FEM Ths nots ar prpard by Dr. Cünyt Srt http://www.m.mtu.du.tr/popl/cunyt

More information

Volterra Kernel Estimation for Nonlinear Communication Channels Using Deterministic Sequences

Volterra Kernel Estimation for Nonlinear Communication Channels Using Deterministic Sequences 1 Voltrra Krnl Estimation for Nonlinar Communication Channls Using Dtrministic Squncs Endr M. Ekşioğlu and Ahmt H. Kayran Dpartmnt of Elctrical and Elctronics Enginring, Istanbul Tchnical Univrsity, Istanbul,

More information

Robust surface-consistent residual statics and phase correction part 2

Robust surface-consistent residual statics and phase correction part 2 Robust surfac-consistnt rsidual statics and phas corrction part 2 Ptr Cary*, Nirupama Nagarajappa Arcis Sismic Solutions, A TGS Company, Calgary, Albrta, Canada. Summary In land AVO procssing, nar-surfac

More information

Detection of Energetic Particles by a Network of HF Propagation Paths in Alaska

Detection of Energetic Particles by a Network of HF Propagation Paths in Alaska Dtction of Enrgtic Particls by a twork of HF Propagation Paths in Alaska A.Y. Wong* HIPAS Obsrvatory, Fairbanks, AK and Dpt of Physics and Astronomy, UCLA *With th assistanc of G. Rosnthal, J. Pau, E.

More information