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

Size: px
Start display at page:

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

Transcription

1 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 Sihm ISECS Rout Mnzl Chakr km 0.5 BP 868, 308 Sfax, Tunisia chaabouni sihm@yahoo.fr Noura Sllami ISECS Rout Mnzl Chakr km 0.5 BP 868, 308 Sfax, Tunisia noura.sllami@iscs.rnu.tn Alin Roumy IRISA-INRIA Campus d Bauliu 3504 Rnns Cdx, Franc alin.roumy@irisa.fr ABSTRACT In this papr, w considr a transmission of M-Phas Shift Kying (M-PSK) symbols with Gray mapping ovr a frquncy slctiv channl. W propos to study analytically th impact of a priori information (providd for instanc by a dcodr in a turbo qualizr) on th maximum a postriori (MAP) qualizr prformanc. W driv analytical xprssions of th bit rror probability at th output of th qualizr. Simulations show that th analytical xprssions approximat wll th bit rror rat () at th output of th MAP qualizr at high signal to nois ratio ().. INTRODUCTION Th high data rat communication systms ar impaird by intrsymbol intrfrnc (ISI). To combat th ffcts of ISI, an qualizr has to b usd. Th optimal soft-input soft-output qualizr, that achivs minimum bit rror rat (), is basd on th maximum a postriori (MAP) critrion. In this papr, w considr th cas whr th M-Phas Shift Kying (M-PSK) modulation (with M = q, for q ) is usd and th MAP qualizr has a priori information on th transmittd data. Th a priori information ar providd by anothr modul in th rcivr, for instanc a dcodr in a turbo-qualizr []. In a turbo-qualizr, th qualizr and th dcodr xchang xtrinsic information and us thm as a priori in ordr to improv thir prformanc. In [], th authors studid analytically th impact of a priori information on th MAP qualizr prformanc in th cas of Binary Phas Shift Kying (BPSK) modulation (M = ). Th aim of our papr is to gnraliz th study of [] to th cas of M-PSK modulation. To do this, w driv analytical approximat xprssions of th at th output of th MAP qualizr. Simulations show that ths xprssions approximat wll th at th output of th MAP qualizr at high. This papr is organizd as follows. In sction, w giv th systm modl. In sction 3, w driv analytical xprssions of th at th output of th MAP qualizr. In sction 4, w giv simulation rsults for 8-PSK and 6-PSK modulations. Throughout this papr matrics ar uppr cas and vctors ar undrlind lowr cas. Th oprator (.) T dnots transposition, and R(.) rprsnts th ral valu.. SYSTEM MODEL W considr a data transmission systm ovr a frquncy slctiv channl. W assum that transmissions ar organizd into bursts of T symbols and th channl is invariant during on burst. Th channl is sprad ovr L symbols. Th input information bit squnc b = (b q( L),...,b (qt ) ) T, is mappd to a squnc of M-PSK symbols with Gray mapping whr M = q, and q. Th basband signal rcivd and sampld at th symbol rat at tim k is: L y k = h i x k i + n k, () i=0 whr h i, rprsnts th i th complx channl tap gain, x k, for L k T, ar th transmittd symbols, n k ar modld as indpndnt random variabls of a complx whit Gaussian nois with zro man and varianc σ, with normal probability dnsity function (pdf) N C ( 0,σ ) whr N C ( α,σ ) dnots a complx Gaussian distribution with man α and varianc σ. Equation () can b rwrittn as follows: y = Hx + n, whr x = (x L,...,x T ) T is th vctor of transmittd symbols, n = (n 0,...,n T ) T is th Gaussian nois vctor, y = (y 0,..., y T ) T is th vctor of th output symbols and H is a T (T + L ) Toplitz matrix dfind as: h L... h h H = L... h () h L... h 0 W assum that th channl is normalizd: L i=0 h i =. In this sction, w considr th cas whr no a priori information is providd to th qualizr. Th data stimat according to th MAP squnc critrion (or to th Maximum Liklihood (ML) critrion, sinc thr is no a priori) is givn by: x = argmin u ( y Hu : u A (T +L ) ), whr A is th symbol alphabt. An rror occurs if th stimatd squnc x is diffrnt from th tru squnc x. Lt us dnot = x x th rsulting rror vctor. A subvnt ξ of th rror vnt is that x is bttr than x in th sns of th ML mtric: ξ : y H x y Hx, W now procd to driv a lowr bound on th of th qualizr. This can b don by computing th xact rror probability of a gni aidd qualizr that has som sid information about th snt squnc. Mor prcisly, w considr th cas whr th rcivr has sid information (from a gni) that on of th two squncs x or x was transmittd. Whn th gni aidd qualizr has this sid information, th pairwis rror probability that it chooss x instad of x is givn by [3]: ( ε P x, x = Q ), (3) 007 EURASIP 357

2 whr ε = H, and Q(α) = ( ) 5th Europan Signal Procssing Confrnc π xp y (EUSIPCO 007), Poznan, dy. Proposition Poland, Sptmbr Suppos3-7, w hav 007, acopyright transmission by EURASIP of M-PSK symbols ovr a frquncy slctiv channl dfind by a Toplitz ma- α trix H and with a complx AWGN of varianc σ. Considr that th MAP qualizr has sid information (from a gni) that on of th two squncs x or x was transmittd and has a priori obsrvations modld as outputs of an AWGN channl with varianc. Thn, th pairwis rror probability that it chooss x instad of x is: Lt us assum that th gni tlls th rcivr that it has to choos btwn th tru squnc x and anothr squnc x, such that (3) is maximal i.. such that th distanc ε is minimal. W now procd to comput th xact rror probability for this gni aidd rcivr. Lt E min b th st of all achiving th minimum valu of ε. Lt π b th probability that th input squnc x will b such that x = x+ is an allowabl input squnc for this. π can b intrprtd as th probability that th data squnc x is compatibl with. Thn, th probability that th gni aidd qualizr maks an rror is min ε π Q E min In ordr to obtain a lowr bound on th, w assum that is mad of m() non-zro conscutiv symbols, th othr symbols bing zro. Othr saying, w assum that thr xists an intrval of siz m() such that all th symbols of x ar diffrnt from th corrsponding symbols of x whil th prcding symbol and th following on ar th sam. m() is rfrrd to as th wight of th rror squnc in th following. Morovr, w rmark that thr is at last on rronous bit pr rronous symbol. Thrfor, whn th qualizr has no sid information, th P is lowr boundd by th probability achivd by th gni aidd qualizr: min ε P m()π Q E min As will b shown by simulations, this lowr bound is a good approximation of th rror probability at high and for a Gray mapping. This can b xplaind by th fact that at high and for a Gray mapping, th union bound (uppr bound) and th abov drivd lowr bound ar qual. Our goal is to find an approximation of th at th output of th MAP qualizr with a priori information. 3. PERFORMANCE ANALYSIS In this sction, w propos to valuat th impact of th a priori information on th MAP qualizr prformanc whn a M-PSK modulation with Gray mapping is usd. Th study will b don for th qualizr using th MAP squnc critrion. It holds for th MAP symbol qualizr using th BCJR algorithm [4] sinc th two qualizrs hav almost th sam prformanc as obsrvd in [5,pag 84]. W assum that channls ar prfctly known at th rcivr. Morovr, w suppos that a priori obsrvations at th input of th qualizr ar modld as outputs of an additiv whit Gaussian nois (AWGN) channl. This is a usual assumption in th analyss of itrativ rcivrs [6]. Ths a priori obsrvations on bits b l, for q( L) l qt, ar: z l = b l + w l, whr w l ar indpndnt random variabls of a ral whit Gaussian nois with zro man and varianc with normal pdf N(0, ), whr N ( α,σ ) dnots a ral Gaussian distribution with man α and varianc σ. Thn, th a priori Log Liklihood Ratios (LLRs) ar: LLR(b l ) = log P(z l b l = ) P(z l b l = ) = z l. Thus, ths LLRs can b modld as indpndnt and idntically ( distributd ) random variabls with th conditional pdf N bl, 4 (with b l th transmittd bit). 007 EURASIP 358 P x, x = Q ( ε + m b ()µ ), (4) whr ε = H, = x x is th symbol rror vctor, m() is th wight in symbols of, m b () is th wight in bits of (m() m b () qm()) and µ = σ σ a. Th proof of proposition is givn in th Appndix. Hr again w assum that th gni always chooss a squnc ˆx that maximizs th pairwis rror probability (4). LtE min b th st of all achiving th minimum valu of ε + m b ()µ, π b th probability that th input squnc x will b such that x = x + is an allowabl input squnc. Thn, th probability that th gni aidd qualizr chooss ( an allowabl squnc x instad of x is Emin π Q (min ε + m b ()µ )). Corollary W considr a M-PSK modulation with Gray mapping. Th at th output of th MAP qualizr without gni, using th a priori information can b approximatd by: ( P m()π Q (min ε + m()µ )), (5) E min whr m() is th numbr of (conscutiv) non zro symbols in. Proof of corollary : For th MAP qualizr without gni, th is lowr boundd by th probability achivd by th gni aidd qualizr: ( m b ()π Q (min ε + m b ()µ )). E min In addition, sinc w us a Gray mapping, w furthr assum that thr is on rronous bit pr rronous symbol, s.t. m b () m(). Simulations show that this assumption bcoms tru at high. Morovr, at high th union bound (uppr bound) and th lowr bound ar qual. Thrfor, th lowr bound of th bcoms an approximation as writtn in (5). In ordr to valuat th xprssion (5), an xhaustiv sarch has to b prformd ovr all possibl rror squncs. W propos to rduc this xhaustiv sarch and to rstrict ourslf to th cas of rror squncs of symbol wight or. Simulations will show that this provids rliabl approximations of th ovrall. In th following, w considr diffrnt cass according to th valu of µ. Corollary Lt d = min ε and d = min ε. If th : m()= : m()= a priori information is unrliabl (i.. d > d and µ µ lim = d d ), th at th output of th MAP qualizr can b approximatd by: ( P π Q d ), + 4µ (6)

3 whr π 5th is Europan th probability Signal Procssing that w can Confrnc find pair(eusipco of squncs 007), Poznan, Poland, Sptmbr 3-7, 007, copyright by EURASIP compatibl with rror squncs of (symbol) wight. Mor Tabl 3: µ lim valus for 8-PSK modulation prcisly π = E π and E is th st of (symbol) wight channl3 channl4 channl3c squncs s.t. ε = d. µ lim On th othr hand, if th information is rliabl (i.. d > d 0 and µ > µ lim or if d d ), th at th output of th MAP qualizr can b approximatd by: ( P Q d ), + µ (7) Proof of corollary : Th valu of µ lim rsults from th quality btwn quations (6) and (7). Whn th a priori information at th input of th MAP qualizr is unrliabl (i.. µ µ lim ), rrors occur in bursts. Thus, w do not considr isolatd rrors and w look for th maximum of (5) for m(). Simulations show that th minimum valu of ε + m()µ is obtaind for rror squnc of wight (i.. m() = and ε = d ). Thrfor th is approximatd by (6). Th valus of π for th diffrnt modulations can b found by an xhaustiv sarch and ar givn in Tabl. In th cas of rliabl a priori information (i.. µ > µ lim ), a priori obsrvations hav mor influnc on th dtction than channl obsrvations and most of th rrors ar isolatd. Thrfor, m() = and ε = d. In this cas for all modulations, π = {: m()= and ε =d } π is qual to, which lads to (7). Dpnding on µ, w gt ithr (6) or (7). W dtrmin a thrshold µ lim as th valu of µ whn (6) quals (7). It follows that µ µ lim corrsponds to th cas with unrliabl a priori and µ > µ lim to th cas with rliabl a priori. Tabl : π valus whn th a priori information at th input of th MAP qualizr ar unrliabl BPSK QPSK 8-PSK 6-PSK π / 3/4 3/8 3/6 4. SIMULATION RESULTS In this sction, w propos to validat th analysis by simulations. In th simulations, th modulation usd is ithr a 8-PSK or a 6-PSK using Gray mapping and th channl is assumd to b constant. W provid th MAP qualizr with a priori information on th transmittd bits b l modld as indpndnt and idntically distributd random variabls with th conditional pdf N( b l, 4 ). W considr diffrnt channls. Figurs, and 3 rprsnt rspctivly th with rspct to th at th output of th MAP qualizr with 8-PSK modulation, for channl3, channl4 and channl3c with impuls rsponss: channl3 = (0.5, 0.7, 0.5), channl4 = (0.37,0.6, 0.6,0.37) and channl3c = ( j, j, j). Tabl givs th valus of d and d for ach channl. For all ths channls, w hav d > d. Th limit valus µ lim ar givn in Tabl 3. Tabl : d and d valus for 8-PSK modulation channl3 channl4 channl3c d d Figurs 4 and 5 rprsnt th with rspct to th at th output of th MAP qualizr with 6-PSK modulation rspctivly for channl3 and channlcomp with impuls rsponss: channl3 = (0.5, 0.7, 0.5) and channlcomp = Figur : vrsus : comparison of th qualizr prformanc curvs) for channl3 and 8-PSK modulation ( j, j, j). Tabl 4 givs th valus of d and d for ach channl. For all ths channls, w hav d > d. Th limit valus µ lim ar givn in Tabl 5. Tabl 4: d and d valus for 6-PSK modulation channl3 channlcomp d d In all figurs, ach curv is obtaind whil th ratio µ is kpt constant. Th solid lins indicat th qualizr prformanc givn by simulations. Th dottd lins ar obtaind by considring th analytical approximat xprssions calculatd in th prvious sction. W notic that th thortical curvs approximat wll th. This approximation bcoms bttr at high (for low valus of ). W can also dduc that th approximation is mor accurat for 8-PSK than for 6-PSK, sinc th assumption that thr is on rronous bit pr rronous symbol is bttr validatd for a 8-PSK modulation. 5. CONCLUSION In this papr, w considrd a transmission of M-PSK symbols ovr a frquncy slctiv channl. W proposd to study analytically th impact of a priori information on th MAP qualizr prformanc. W gav an approximation of th rror probability at th output of th MAP qualizr. Simulation rsults showd that th analytical xprssions giv a good approximation of th qualizr prformanc. Th aim of this work is to prform in th futur th analytical convrgnc analysis of itrativ rcivrs with MAP qualization. 6. APPENDIX: PROOF FOR PROPOSITION W rcall that th output of th channl during a burst is th T complx vctor y = (y 0,...,y T ) T dfind as: y = Hx + n, 007 EURASIP 359

4 0 5th Europan Signal Procssing Confrnc (EUSIPCO 007), Poznan, 0Poland, Sptmbr 3-7, 007, copyright by EURASIP Figur : vrsus : comparison of th qualizr prformanc curvs) for channl4 and 8-PSK modulation Figur 4: vrsus : comparison of th qualizr prformanc curvs) for channl3 and 6-PSK modulation Figur 3: vrsus : comparison of th qualizr prformanc curvs) for channl3c and 8-PSK modulation Figur 5: vrsus : comparison of th qualizr prformanc curvs) for channlcomp and 6-PSK modulation whr x = (x L,...,x T ) T is th (T + L ) vctor of transmittd symbols, n = (n 0,...,n T ) T is a complx whit Gaussian nois vctor with zro man and varianc σ and H is th T (T + L ) channl matrix givn by (). Th ral vctor of a priori obsrvations z = (z q( L),...,z (qt ) ) T on th transmittd bits is dfind as: z = b + w, whr w = (w q( L),...,w (qt ) ) T is a ral whit Gaussian nois vctor with zro man and varianc and b = (b q( L),...,b (qt ) ) T is th vctor of transmittd bits. Taking into account th a priori information, th a postriori Tabl 5: µ lim valus for 6-PSK modulation channl3 channlcomp µ lim probability of th squnc x is givn by: P ( x y,z ) ( y Hx ) ( ) z b xp σ xp a. As in th cas of no a priori information, w considr an rror vnt ξ. This rror vnt is that x is bttr than x in th sns of th MAP squnc mtric: ξ : y H x + σ a z b y Hx + σ a z b, (8) Lt = x x and a = b b b rspctivly th symbol rror 007 EURASIP 360

5 vctor and 5th theuropan bit rrorsignal vctor. Procssing W hav: Confrnc (EUSIPCO 007), Poznan, sinc th Poland, numbr Sptmbr of rronous 3-7, 007, bit copyright pr rronous by EURASIP symbol is b- y H x y Hx twn and q. Th vctor a has m b () componnts qual to (9) = y Hx H ± and th othrs qual to zro. Thus, w can rplac a by y Hx 4m b () and w obtain: = H R( y Hx,H ( ) = ε P x, x = Q ε + m b ()µ ). R( n,ε ), whr ε = H. In addition: z b z b = z b a z b = a z b,a W obtain using (8), (9) and (0): = a w,a. (0) ξ : ε + µ a R( n,ε ) + µ w,a, whr µ = σ σ a. W not χ = R( n,ε ) + µ w,a. W can writ that χ N (0, ( ε + µ a )). Thus, whn th gni aidd qualizr is providd with a priori information, th pairwis rror probability that it chooss x instad of x is givn by: ( ) P x, x = Q ε + µ a. Lt m b () b th wight of th bit rror vctor, and m() th wight of th symbol rror vctor with m() m b () qm() REFERENCES [] C.Douillard, M.Jzqul, C.Brrou, A.Picart, P.Didir, A.Glaviux, Itrativ corrction of intrsymbol intrfrnc: Turbo-qualization, Europ. Trans. On Tlcomm., vol. 6, pp , 995. [] N.Sllami, A.Roumy, I.Fijalkow, Th impact of both a priori information and channl stimation rrors on th MAP qualizr prformanc, IEEE Transactions on Signal Procssing, vol. 54, No 7, pp , July 006. [3] G.D.Forny, Jr., Lowr bounds on rror probability in th prsnc of larg intrsymbol intrfrnc, IEEE Transactions on Communications, pp , Fbruary 97. [4] L.R.Bahl, J.Cock, F.Jlink, J.Raviv, Optimal dcoding of linar cods for minimizing symbol rror rat, IEEE Trans. Inf. Thory, vol.it-3, pp , March 974. [5] S.Bndtto, E.Bigliri, Principls of digital transmission with wirlss applications, kluwr/plnum, Nw York 999. [6] S.Tn Brink, Convrgnc of itrativ dcoding, IEEE Elctronic Lttrs, vol. 35, pp , May EURASIP 36

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

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by D. Klain Vrsion 207.0.05 Corrctions and commnts ar wlcom. Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix A A k I + A + k!

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

The Matrix Exponential

The Matrix Exponential Th Matrix Exponntial (with xrciss) by Dan Klain Vrsion 28928 Corrctions and commnts ar wlcom Th Matrix Exponntial For ach n n complx matrix A, dfin th xponntial of A to b th matrix () A A k I + A + k!

More information

EXST Regression Techniques Page 1

EXST Regression Techniques Page 1 EXST704 - Rgrssion Tchniqus Pag 1 Masurmnt rrors in X W hav assumd that all variation is in Y. Masurmnt rror in this variabl will not ffct th rsults, as long as thy ar uncorrlatd and unbiasd, sinc thy

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

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

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

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

Einstein Equations for Tetrad Fields

Einstein Equations for Tetrad Fields Apiron, Vol 13, No, Octobr 006 6 Einstin Equations for Ttrad Filds Ali Rıza ŞAHİN, R T L Istanbul (Turky) Evry mtric tnsor can b xprssd by th innr product of ttrad filds W prov that Einstin quations for

More information

Frequency Correction

Frequency Correction Chaptr 4 Frquncy Corrction Dariush Divsalar Ovr th yars, much ffort has bn spnt in th sarch for optimum synchronizion schms th ar robust and simpl to implmnt [1,2]. Ths schms wr drivd basd on maximum-liklihood

More information

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches. Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M

More information

Strong Converse, Feedback Channel Capacity. and Hypothesis Testing. Journal of the Chinese Institute of Engineers, to appear November 1995.

Strong Converse, Feedback Channel Capacity. and Hypothesis Testing. Journal of the Chinese Institute of Engineers, to appear November 1995. Strong Convrs, Fdback Channl Capacity and Hypothsis Tsting Po-Ning Chn Computr & Communication Rsarch Laboratoris Industrial Tchnology Rsarch Institut Taiwan 30, Rpublic of China Fady Alajaji Dpartmnt

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

Section 11.6: Directional Derivatives and the Gradient Vector

Section 11.6: Directional Derivatives and the Gradient Vector Sction.6: Dirctional Drivativs and th Gradint Vctor Practic HW rom Stwart Ttbook not to hand in p. 778 # -4 p. 799 # 4-5 7 9 9 35 37 odd Th Dirctional Drivativ Rcall that a b Slop o th tangnt lin to th

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

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 0 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat th

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

That is, we start with a general matrix: And end with a simpler matrix:

That is, we start with a general matrix: And end with a simpler matrix: DIAGON ALIZATION OF THE STR ESS TEN SOR INTRO DUCTIO N By th us of Cauchy s thorm w ar abl to rduc th numbr of strss componnts in th strss tnsor to only nin valus. An additional simplification of th strss

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

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

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

Computing and Communications -- Network Coding

Computing and Communications -- Network Coding 89 90 98 00 Computing and Communications -- Ntwork Coding Dr. Zhiyong Chn Institut of Wirlss Communications Tchnology Shanghai Jiao Tong Univrsity China Lctur 5- Nov. 05 0 Classical Information Thory Sourc

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

Addition of angular momentum

Addition of angular momentum Addition of angular momntum April, 07 Oftn w nd to combin diffrnt sourcs of angular momntum to charactriz th total angular momntum of a systm, or to divid th total angular momntum into parts to valuat

More information

Solution of Assignment #2

Solution of Assignment #2 olution of Assignmnt #2 Instructor: Alirza imchi Qustion #: For simplicity, assum that th distribution function of T is continuous. Th distribution function of R is: F R ( r = P( R r = P( log ( T r = P(log

More information

Supplementary Materials

Supplementary Materials 6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic

More information

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK

Data Assimilation 1. Alan O Neill National Centre for Earth Observation UK Data Assimilation 1 Alan O Nill National Cntr for Earth Obsrvation UK Plan Motivation & basic idas Univariat (scalar) data assimilation Multivariat (vctor) data assimilation 3d-Variational Mthod (& optimal

More information

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional

Chapter 13 GMM for Linear Factor Models in Discount Factor form. GMM on the pricing errors gives a crosssectional Chaptr 13 GMM for Linar Factor Modls in Discount Factor form GMM on th pricing rrors givs a crosssctional rgrssion h cas of xcss rturns Hors rac sting for charactristic sting for pricd factors: lambdas

More information

Estimation of apparent fraction defective: A mathematical approach

Estimation of apparent fraction defective: A mathematical approach Availabl onlin at www.plagiarsarchlibrary.com Plagia Rsarch Library Advancs in Applid Scinc Rsarch, 011, (): 84-89 ISSN: 0976-8610 CODEN (USA): AASRFC Estimation of apparnt fraction dfctiv: A mathmatical

More information

Homework #3. 1 x. dx. It therefore follows that a sum of the

Homework #3. 1 x. dx. It therefore follows that a sum of the Danil Cannon CS 62 / Luan March 5, 2009 Homwork # 1. Th natural logarithm is dfind by ln n = n 1 dx. It thrfor follows that a sum of th 1 x sam addnd ovr th sam intrval should b both asymptotically uppr-

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

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

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

There is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real.

There is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real. Midtrm #, Physics 37A, Spring 07. Writ your rsponss blow or on xtra pags. Show your work, and tak car to xplain what you ar doing; partial crdit will b givn for incomplt answrs that dmonstrat som concptual

More information

Bit-Loading Algorithms for OFDM with Adaptive Cyclic Prefix Length in PLC Channels

Bit-Loading Algorithms for OFDM with Adaptive Cyclic Prefix Length in PLC Channels Bit-Loading Algorithms for OFD with Adaptiv Cyclic Prfix Lngth in PLC Channls Salvator D Alssandro (), Andra. Tonllo (), and Lutz Lamp (3) (,) DIEG - Univrsità di Udin, Udin, Italy, -mail: salvator.dalssandro@uniud.it,

More information

Calculus II (MAC )

Calculus II (MAC ) Calculus II (MAC232-2) Tst 2 (25/6/25) Nam (PRINT): Plas show your work. An answr with no work rcivs no crdit. You may us th back of a pag if you nd mor spac for a problm. You may not us any calculators.

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

Gaussian and Flat Rayleigh Fading Channel Influences on PAPR Distribution in MIMO-OFDM Systems

Gaussian and Flat Rayleigh Fading Channel Influences on PAPR Distribution in MIMO-OFDM Systems Gaussian and Flat Rayligh Fading Channl Influncs on PAPR Distribution in MIMO-OFDM Systms Basl Rihawi and Yvs Louët IETR/Supélc - Campus d Rnns Avnu d la Boulai, BP 87, 355 Csson-Sévigné, Franc Tlphon:

More information

Differential Equations

Differential Equations UNIT I Diffrntial Equations.0 INTRODUCTION W li in a world of intrrlatd changing ntitis. Th locit of a falling bod changs with distanc, th position of th arth changs with tim, th ara of a circl changs

More information

ARIMA Methods of Detecting Outliers in Time Series Periodic Processes

ARIMA Methods of Detecting Outliers in Time Series Periodic Processes Articl Intrnational Journal of Modrn Mathmatical Scincs 014 11(1): 40-48 Intrnational Journal of Modrn Mathmatical Scincs Journal hompag:www.modrnscintificprss.com/journals/ijmms.aspx ISSN:166-86X Florida

More information

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator. Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r

More information

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1 F110 Spktrala transformr för Mdia Solutions to Stiglitz, Chaptr 1 Prfac This documnt contains solutions to slctd problms from Kn Stiglitz s book: A Digital Signal Procssing Primr publishd by Addison-Wsly.

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

Collisions between electrons and ions

Collisions between electrons and ions DRAFT 1 Collisions btwn lctrons and ions Flix I. Parra Rudolf Pirls Cntr for Thortical Physics, Unirsity of Oxford, Oxford OX1 NP, UK This rsion is of 8 May 217 1. Introduction Th Fokkr-Planck collision

More information

Carrier frequency estimation. ELEC-E5410 Signal processing for communications

Carrier frequency estimation. ELEC-E5410 Signal processing for communications Carrir frquncy stimation ELEC-E54 Signal procssing for communications Contnts. Basic systm assumptions. Data-aidd DA: Maximum-lilihood ML stimation of carrir frquncy 3. Data-aidd: Practical algorithms

More information

2.3 Matrix Formulation

2.3 Matrix Formulation 23 Matrix Formulation 43 A mor complicatd xampl ariss for a nonlinar systm of diffrntial quations Considr th following xampl Exampl 23 x y + x( x 2 y 2 y x + y( x 2 y 2 (233 Transforming to polar coordinats,

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

Linear Non-Gaussian Structural Equation Models

Linear Non-Gaussian Structural Equation Models IMPS 8, Durham, NH Linar Non-Gaussian Structural Equation Modls Shohi Shimizu, Patrik Hoyr and Aapo Hyvarinn Osaka Univrsity, Japan Univrsity of Hlsinki, Finland Abstract Linar Structural Equation Modling

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

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

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

Limiting value of higher Mahler measure

Limiting value of higher Mahler measure Limiting valu of highr Mahlr masur Arunabha Biswas a, Chris Monico a, a Dpartmnt of Mathmatics & Statistics, Txas Tch Univrsity, Lubbock, TX 7949, USA Abstract W considr th k-highr Mahlr masur m k P )

More information

A Low-Cost and High Performance Solution to Frequency Estimation for GSM/EDGE

A Low-Cost and High Performance Solution to Frequency Estimation for GSM/EDGE A Low-Cost and High Prformanc Solution to Frquncy Estimation for GSM/EDGE Wizhong Chn Lo Dhnr fwc@frscal.com ld@frscal.com 5-996- 5-996-75 77 Wst Parmr Ln 77 Wst Parmr Ln Austin, TX7879 Austin, TX7879

More information

Chapter 10. The singular integral Introducing S(n) and J(n)

Chapter 10. The singular integral Introducing S(n) and J(n) Chaptr Th singular intgral Our aim in this chaptr is to rplac th functions S (n) and J (n) by mor convnint xprssions; ths will b calld th singular sris S(n) and th singular intgral J(n). This will b don

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

Sara Godoy del Olmo Calculation of contaminated soil volumes : Geostatistics applied to a hydrocarbons spill Lac Megantic Case

Sara Godoy del Olmo Calculation of contaminated soil volumes : Geostatistics applied to a hydrocarbons spill Lac Megantic Case wwwnvisol-canadaca Sara Godoy dl Olmo Calculation of contaminatd soil volums : Gostatistics applid to a hydrocarbons spill Lac Mgantic Cas Gostatistics: study of a PH contamination CONTEXT OF THE STUDY

More information

Higher order derivatives

Higher order derivatives Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of

More information

Economics 201b Spring 2010 Solutions to Problem Set 3 John Zhu

Economics 201b Spring 2010 Solutions to Problem Set 3 John Zhu Economics 20b Spring 200 Solutions to Problm St 3 John Zhu. Not in th 200 vrsion of Profssor Andrson s ctur 4 Nots, th charactrization of th firm in a Robinson Cruso conomy is that it maximizs profit ovr

More information

Sequential Decentralized Detection under Noisy Channels

Sequential Decentralized Detection under Noisy Channels Squntial Dcntralizd Dtction undr Noisy Channls Yasin Yilmaz Elctrical Enginring Dpartmnt Columbia Univrsity Nw Yor, NY 1007 Email: yasin@.columbia.du Gorg Moustaids Dpt. of Elctrical & Computr Enginring

More information

Random Access Techniques: ALOHA (cont.)

Random Access Techniques: ALOHA (cont.) Random Accss Tchniqus: ALOHA (cont.) 1 Exampl [ Aloha avoiding collision ] A pur ALOHA ntwork transmits a 200-bit fram on a shard channl Of 200 kbps at tim. What is th rquirmnt to mak this fram collision

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

What are those βs anyway? Understanding Design Matrix & Odds ratios

What are those βs anyway? Understanding Design Matrix & Odds ratios Ral paramtr stimat WILD 750 - Wildlif Population Analysis of 6 What ar thos βs anyway? Undrsting Dsign Matrix & Odds ratios Rfrncs Hosmr D.W.. Lmshow. 000. Applid logistic rgrssion. John Wily & ons Inc.

More information

1973 AP Calculus AB: Section I

1973 AP Calculus AB: Section I 97 AP Calculus AB: Sction I 9 Minuts No Calculator Not: In this amination, ln dnots th natural logarithm of (that is, logarithm to th bas ).. ( ) d= + C 6 + C + C + C + C. If f ( ) = + + + and ( ), g=

More information

cycle that does not cross any edges (including its own), then it has at least

cycle that does not cross any edges (including its own), then it has at least W prov th following thorm: Thorm If a K n is drawn in th plan in such a way that it has a hamiltonian cycl that dos not cross any dgs (including its own, thn it has at last n ( 4 48 π + O(n crossings Th

More information

ECE602 Exam 1 April 5, You must show ALL of your work for full credit.

ECE602 Exam 1 April 5, You must show ALL of your work for full credit. ECE62 Exam April 5, 27 Nam: Solution Scor: / This xam is closd-book. You must show ALL of your work for full crdit. Plas rad th qustions carfully. Plas chck your answrs carfully. Calculators may NOT b

More information

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding... Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg

More information

Unconventional Behavior of the Noisy Min-Sum Decoder over the Binary Symmetric Channel

Unconventional Behavior of the Noisy Min-Sum Decoder over the Binary Symmetric Channel Unconvntional Bhavior of th Noisy Min-Sum Dcodr ovr th Binary Symmtric Channl Christian L. Kamni Ngassa,#, Valntin Savin, David Dclrcq # CEA-LETI, Minatc Campus, Grnobl, Franc, {christian. kamningassa,

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

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH. C:\Dallas\0_Courss\03A_OpSci_67\0 Cgh_Book\0_athmaticalPrliminaris\0_0 Combath.doc of 8 COPUTER GENERATED HOLOGRAS Optical Scincs 67 W.J. Dallas (onday, April 04, 005, 8:35 A) PART I: CHAPTER TWO COB ATH

More information

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals. Chaptr 7 Th Hydrogn Atom Background: W hav discussd th PIB HO and th nrgy of th RR modl. In this chaptr th H-atom and atomic orbitals. * A singl particl moving undr a cntral forc adoptd from Scott Kirby

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

Detection Algorithms for Physical Network Coding

Detection Algorithms for Physical Network Coding 01 7th Intrnational ICST Confrnc on Communications and Ntworing in China (CINCOM Dtction lgorithms for Physical Ntwor Coding Chngang Pan, Jianjun Liu, Zhnping u China Mobil sarch Institut ijing, China

More information

Principles of Humidity Dalton s law

Principles of Humidity Dalton s law Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid

More information

Mathematics. Complex Number rectangular form. Quadratic equation. Quadratic equation. Complex number Functions: sinusoids. Differentiation Integration

Mathematics. Complex Number rectangular form. Quadratic equation. Quadratic equation. Complex number Functions: sinusoids. Differentiation Integration Mathmatics Compl numbr Functions: sinusoids Sin function, cosin function Diffrntiation Intgration Quadratic quation Quadratic quations: a b c 0 Solution: b b 4ac a Eampl: 1 0 a= b=- c=1 4 1 1or 1 1 Quadratic

More information

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES Eduard N. Klnov* Rostov-on-Don, Russia Th articl considrs phnomnal gomtry figurs bing th carrirs of valu spctra for th pairs of th rmaining additiv

More information

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero. SETION 6. 57 6. Evaluation of Dfinit Intgrals Exampl 6.6 W hav usd dfinit intgrals to valuat contour intgrals. It may com as a surpris to larn that contour intgrals and rsidus can b usd to valuat crtain

More information

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming

CPSC 665 : An Algorithmist s Toolkit Lecture 4 : 21 Jan Linear Programming CPSC 665 : An Algorithmist s Toolkit Lctur 4 : 21 Jan 2015 Lcturr: Sushant Sachdva Linar Programming Scrib: Rasmus Kyng 1. Introduction An optimization problm rquirs us to find th minimum or maximum) of

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

Density Evolution and Functional Threshold. for the Noisy Min-Sum Decoder

Density Evolution and Functional Threshold. for the Noisy Min-Sum Decoder Dnsity Evolution and Functional Thrshold 1 for th Noisy Min-Sum Dcodr (Extndd Vrsion arxiv:145.6594v1 [cs.it] 26 May 214 Christian L. Kamni Ngassa,#, Valntin Savin, Elsa Dupraz #, David Dclrcq # CEA-LETI,

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

Comparison of bit error rate and convergence of four different iterative receivers for wireless OFDM-CDM

Comparison of bit error rate and convergence of four different iterative receivers for wireless OFDM-CDM Int. J. Elctron. Commun. (AEÜ) 59 (2005) 66 76 www.lsvir.d/au Comparison of bit rror rat convrgnc of four diffrnt itrativ rcivrs for wirlss OFDM-CDM Fridrich Sanzi Businss Unit Logistics, Luz lctronic

More information

Engineering 323 Beautiful HW #13 Page 1 of 6 Brown Problem 5-12

Engineering 323 Beautiful HW #13 Page 1 of 6 Brown Problem 5-12 Enginring Bautiful HW #1 Pag 1 of 6 5.1 Two componnts of a minicomputr hav th following joint pdf for thir usful liftims X and Y: = x(1+ x and y othrwis a. What is th probability that th liftim X of th

More information

2008 AP Calculus BC Multiple Choice Exam

2008 AP Calculus BC Multiple Choice Exam 008 AP Multipl Choic Eam Nam 008 AP Calculus BC Multipl Choic Eam Sction No Calculator Activ AP Calculus 008 BC Multipl Choic. At tim t 0, a particl moving in th -plan is th acclration vctor of th particl

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

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values Dnamic Macroconomic Thor Prof. Thomas Lux Bifurcation Thor Bifurcation: qualitativ chang in th natur of th solution occurs if a paramtr passs through a critical point bifurcation or branch valu. Local

More information

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott

SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER J. C. Sprott PLP 821 Novmbr 1979 Plasma Studis Univrsity of Wisconsin Ths PLP Rports ar informal and prliminary and as such may contain rrors not yt

More information

Derangements and Applications

Derangements and Applications 2 3 47 6 23 Journal of Intgr Squncs, Vol. 6 (2003), Articl 03..2 Drangmnts and Applications Mhdi Hassani Dpartmnt of Mathmatics Institut for Advancd Studis in Basic Scincs Zanjan, Iran mhassani@iasbs.ac.ir

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

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

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

Errata. Items with asterisks will still be in the Second Printing

Errata. Items with asterisks will still be in the Second Printing Errata Itms with astrisks will still b in th Scond Printing Author wbsit URL: http://chs.unl.du/edpsych/rjsit/hom. P7. Th squar root of rfrrd to σ E (i.., σ E is rfrrd to not Th squar root of σ E (i..,

More information

Uplink channel estimation for multi-user OFDM-based systems

Uplink channel estimation for multi-user OFDM-based systems plink channl stimation for multi-usr OFDM-basd systms Carlos Ribiro *, M. Julia Frnándz-Gtino García, Víctor P. Gil Jiménz Atílio Gamiro* and Ana García Armada Instituto Politécnico d Liria, Morro do Lna,

More information

Analysis and Optimization for Weighted Sum Rate in Energy Harvesting Cooperative NOMA Systems

Analysis and Optimization for Weighted Sum Rate in Energy Harvesting Cooperative NOMA Systems Analysis and Optimization for Wightd Sum Rat in Enrgy Harvsting Cooprativ NOMA Systms Binh Van Nguyn, Quang-Doanh Vu, and Kison Kim arxiv:86.264v [cs.it] 6 Jun 28 Abstract W considr a cooprativ non-orthogonal

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

A. Limits and Horizontal Asymptotes ( ) f x f x. f x. x "±# ( ).

A. Limits and Horizontal Asymptotes ( ) f x f x. f x. x ±# ( ). A. Limits and Horizontal Asymptots What you ar finding: You can b askd to find lim x "a H.A.) problm is asking you find lim x "# and lim x "$#. or lim x "±#. Typically, a horizontal asymptot algbraically,

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

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

2. Laser physics - basics

2. Laser physics - basics . Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"

More information

Problem Set 6 Solutions

Problem Set 6 Solutions 6.04/18.06J Mathmatics for Computr Scinc March 15, 005 Srini Dvadas and Eric Lhman Problm St 6 Solutions Du: Monday, March 8 at 9 PM in Room 3-044 Problm 1. Sammy th Shark is a financial srvic providr

More information