Sequential Decentralized Detection under Noisy Channels

Size: px
Start display at page:

Download "Sequential Decentralized Detection under Noisy Channels"

Transcription

1 Squntial Dcntralizd Dtction undr Noisy Channls Yasin Yilmaz Elctrical Enginring Dpartmnt Columbia Univrsity Nw Yor, NY Gorg Moustaids Dpt. of Elctrical & Computr Enginring Univrsity of Patras 6500 Rion, Grc Xiaodong Wang Elctrical Enginring Dpartmnt Columbia Univrsity Nw Yor, NY Abstract W considr dcntralizd dtction through distributd snsors that prform lvl-triggrd sampling and communicat with a fusion cntr (FC via noisy channls. Each snsor computs its local log-lilihood ratio (LLR, sampls it using th lvl-triggrd sampling, and upon sampling transmits a singl bit to th FC. Upon rciving a bit from a snsor, th FC updats th global LLR and prforms a squntial probability ratio tst (SPRT stp. W driv th fusion ruls undr various typs of channls. W furthr provid nonasymptotic and asymptotic analyss on th avrag dtction dlay for th proposd channl-awar schm, and show that th asymptotic dtction dlay is charactrizd by a KL information numbr. Th dlay analysis facilitats th choic of appropriat signaling schms undr diffrnt channl typs for snding th 1-bit information from snsors to th FC. I. INTRODUCTION In this papr, w considr th dcntralizd dtction problm in which a numbr of snsors communicat to a fusion cntr (FC undr bandwith constraints. Th FC is rsponsibl for maing th final dcision basd on th limitd information it rcivs from th snsors. 1 and, which ar among th arly wors trating th problm, showd th optimality of lilihood ratio tst as a local dcision rul at snsors and a global dcision rul at th FC, rspctivly. Most of th wors on dcntralizd dtction, including th abov mntiond, followd th fixd-samplsiz approach whr th FC mas th global dcision at a fixd tim. On th othr hand, som wors,.g., 3 6, considrd th squntial approach whr th dcision tim of th FC is random. Among thos wors 5, 6 usd squntial probability ratio tst (SPRT both at snsors and th FC. It has bn obsrvd that SPRT rquirs, on avrag, approximatly four tims 7, Pag 109 lss sampls (for Gaussian signals to rach a dcision than th bst fixdsampl-siz tst, for th sam lvl of confidnc. Rlaxing th strict bandwith constraint, it is nown that data fusion (multi-bit mssaging is a much mor powrful tchniqu than dcision fusion (on-bit mssaging, albit it consums highr bandwith. Morovr, th lvl-triggrd samplingbasd squntial dtction schms, rcntly proposd in 5 and 6, ar as powrful as data fusion tchniqus, and at th sam tim thy ar as simpl and bandwith-fficint as dcision fusion tchniqus. In practic, thr ar two sourcs of uncrtainty in a dcntralizd systm, namly th nois in listning channls, corrupting th snsor obsrvations, and th nois in transmission channls, corrupting th mssags rcivd by th FC. Th convntional approach to dcntralizd dtction considrs th formr, but ignors th lattr,.g., 1 6. In othr words, th convntional approach assums idal transmission channls whil applying a fusion rul to th mssags rcivd by th FC. Following th convntional approach, bfor applying a fusion rul, a communication bloc can b indpndntly applid to rcovr th information bits transmittd from snsors. Howvr, this two-stp solution causs prformanc loss du to th data procssing inquality. For an optimal solution, th fusion rul should b channlawar, i.., should us th th nowldg on noisy channls 8. In this papr, w dsign and analyz channl-awar squntial dcntralizd dtction schms basd on lvltriggrd sampling, undr diffrnt typs of discrt and continuous noisy channls. In particular, w first driv channl-awar squntial dtction schms basd on lvltriggrd sampling. W thn prsnt an information thortic framwor to analyz th dcision dlay prformanc of th proposd schms basd on which w provid both nonasymptotic and asymptotic analyss on th dcision dlays undr various typs of channls. Basd on th xprssions of th asymptotic dcision dlays, w also considr appropriat signaling schms undr diffrnt continuous channls to minimiz th asymptotic dlays. Th rmaindr of th papr is organizd as follows. In Sction II, w dscrib th gnral structur of th dcntralizd dtction approach basd on lvl-triggrd sampling with noisy channls btwn snsors and th FC. In Sction III, w driv channl-awar fusion ruls at th FC for various typs of channls. Nxt, w provid analyss on th dcision dlay prformanc for idal channl and noisy channls in Sction IV and Sction V, rspctivly. Finally, th papr is concludd in Sction VI.

2 y 1 b S 1 n zn 1 t 1 ch1 Ii 1(t Î1 i (t Ĩ1 i (t y t y K t I i (t I K i (t S S K b n Îi (t Î K i b K n (t ch chk z n Ĩ i (t z K n Ĩ K i (t FC Fig. 1. A wirlss snsor ntwor with K snsors, and an FC. Snsors procss thir obsrvations {yt }, and transmits information bits {b n}. Thn, th FC, rciving {zn } through wirlss channls, mas a dtction dcision δ T. Ii (t, Î i (t, Ĩ i (t ar th obsrvd, transmittd and rcivd information ntitis rspctivly, which will b dfind in Sction IV. II. SYSTEM DESCRIPTIONS Considr a wirlss snsor ntwor consisting of K snsors ach of which obsrvs a Nyquist-rat sampld discrttim signal {yt : t N}, = 1,..., K. Each snsor computs th log-lilihood ratios (LLR {L t } t of th signal it obsrvs, sampls th LLR squnc using th lvl-triggrd sampling, and thn snds th LLR sampls to th fusion cntr (FC. Th FC thn combins th local LLR information from all snsors, and dcids btwn two hypothss, H 0 and H 1, in a squntial mannr. Obsrvations collctd at th sam snsor, {yt } t, ar assumd to b i.i.d., and in addition obsrvations collctd at diffrnt snsors, {yt }, ar assumd to b indpndnt. Hnc, th local LLR at th -th snsor, L t, and th global LLR, L t, ar computd as L t log f 1 (y 1,..., y t f 0 (y 1,..., y t = L t 1 + l t = δt t ln, (1 and L t = K =1 L t, rspctivly, whr lt log f 1 (y t f0 (y t is th LLR of th sampl yt rcivd at th -th snsor at tim t; fi, i = 0, 1, is th probability dnsity function (pdf of th rcivd signal by th -th snsor undr H i. Th -th snsor sampls L t via lvl-triggrd sampling at a squnc of random sampling tims {t n} n that ar dictatd by L t itslf. Spcifically, th n-th sampl is tan from L t whnvr th accumulatd LLR L t L sinc th last sampling tim tn 1, t n 1 xcds a constant in absolut valu, i.., { } t n min t > t n 1 : L t L t (,, ( n 1 whr t 0 = 0, L 0 = 0. Lt λ n dnot th accumulatd LLR during th n-th intr-sampling intrval, (t n 1, t n, i.., t n λ n lt = L t L n t. (3 n 1 t=t n 1 +1 Immdiatly aftr sampling at t n, as shown in Fig. 1, an information bit b n indicating th thrshold crossd by λ n is transmittd to th FC, i.., b n sign(λ n. (4 Not that ach snsor, in fact, prforms th Wald s wll nown squntial probability ratio tst (SPRT with thrsholds and. SPRT is th optimum squntial tst in th i.i.d. cas in trms of minimizing th avrag dcision dlay 9. At snsor th n-th local SPRT starts at tim t n 1 and nds at tim t n whn th local tst statistic λ n xcds ithr or. This local hypothsis tst producs a local dcision rprsntd by th information bit b n, and inducs local rror probabilitis α and β which ar givn by α P 0 (b n = 1, and β P 1 (b n = 1, (5 rspctivly, whr P i (, i = 0, 1, dnots th probability undr H i. Dnot th rcivd signal at th FC corrsponding to b n as z n cf. Fig. 1. Th FC thn computs th LLR λ n of ach rcivd signal and approximats th global LLR L t as L t N K t =1 λ n with λ n log p 1(z n p 0 (z n, (6 whr Nt is th total numbr of LLR mssags th -th snsor has transmittd up to tim t, and p i (, i = 0, 1, is th pdf of zn undr H i. In particular, suppos that th m-th LLR mssag λ m from any snsor is rcivd at tim t m. Thn at t m, th FC first updats th global LLR as L tm = L tm 1 + λ m. (7 It thn prforms an SPRT stp by comparing L tm with two thrsholds à and B, and applying th following dcision rul H 1, if L tm Ã, δ tm H 0, if L tm B, (8, othrwis. In othr words, it continus to rciv LLR mssags if L tm ( B, Ã. Th thrsholds (Ã, B > 0 ar slctd to satisfy th rror probability constraints P 0 (δ T = H 1 α and P 1 (δ T = H 0 β with qualitis, whr α, β ar targt rror probability bounds, and T min{t > 0 : L t ( B, Ã} (9 is th dtction dlay. With idal channls btwn snsors and th FC, w hav zn = b n, so from (5 w can writ th local LLR λ n = ˆλ n, whr ˆλ n log P1(b n =1 P 0(b n =1 = log 1 β α, if b n = 1, log P1(b n = 1 P 0(b = log β n = 1 1 α, if b n = 1. (10 In this papr, w will assum, as in 5, that th local rror probabilitis {α, β } ar availabl at th FC in ordr to comput th LLR λ n of th rcivd signals. For th cas of idal channls, w us th A and B to dnot th thrsholds in (8, i.., à = A, B = B, and us T to dnot th dcision dlay in (9, i.., T = T. In th cas of noisy channls, th rcivd signal z n is not always idntical to th transmittd bit b n, and thus th LLR λ n of z n can b diffrnt from ˆλ n of b n givn in (10. In th

3 nxt sction, w considr som popular channl modls and giv th corrsponding xprssions for λ n. III. CHANNEL-AWARE FUSION RULES In computing th LLR λ n of th rcivd signal z n, w will ma us of th local snsor rror probabilitis α, β, and th channl paramtrs that charactriz th statistical proprty of th channl. In this papr, w assum sampling (communication tims ar rliably dtctd at th FC undr continuous channls by using high nough signaling lvls at th snsors. Th unrliabl dtction of sampling tims undr continuous channls is analyzd in 10, Sction VI. A. Binary Erasur Channls (BEC Considr binary rasur channls btwn snsors and th FC with rasur probabilitis {ɛ }. Undr BEC, a transmittd bit b n is lost with probability ɛ, and corrctly rcivd at th FC, i.., zn = b n, with probability 1 ɛ. Thn th LLR of zn is givn by λ n = log P1(z n =1 P 0(z n =1 = log 1 β α, if z n = 1, log P1(z n = 1 P 0(z = log β n = 1 1 α, if z n = 1. (11 Not that undr BEC th channl paramtr ɛ is not ndd whn computing th LLR λ n. Not also that in this cas, a rcivd bit bars th sam amount of LLR information as in th idal channl cas, although a transmittd bit is not always rcivd. Hnc, th channl-awar approach coincids with th convntional approach which rlis solly on th rcivd signal. Although th LLR updats in (10 and (11 ar idntical, th fusion ruls undr BEC and idal channls ar not sinc th thrsholds à and B of BEC, du to th information loss, ar in gnral diffrnt from th thrsholds A and B of th idal channl cas. B. Binary Symmtric Channls (BSC Nxt, w considr binary symmtric channls with crossovr probabilitis {ɛ } btwn snsors and th FC. Undr BSC, th transmittd bit b n is flippd, i.., z n = b n, with probability ɛ, and it is corrctly rcivd, i.., z n = b n, with probability 1 ɛ. Th LLR of z n can b computd as λ n(zn = 1 = log P1 1(zn = 1P P 1 1 (z n = 1P 1 1 P 1 0 (z n = 1P P 1 0 (z n = 1P 1 0 = log (1 ɛ (1 β + ɛ β (1 ɛ α + ɛ (1 α ˆβ {}}{ = log 1 (1 ɛ β + ɛ (1 ɛ α + ɛ }{{} ˆα (1 whr P j i, i = 0, 1, j = 1, 1, is th probability undr H i givn b n = j,and {ˆα, ˆβ } ar th ffctiv local rror probabilitis at th FC undr BSC. Similarly w can writ λ n(z n = 1 = log ˆβ 1 ˆα. (13 Not that ˆα > α, ˆβ > β if α < 0.5, β < 0.5,, which w assum tru for > 0. Thus, w hav λ n,bsc < λ n,bec from which w xpct th prformanc loss undr BSC will b highr than that undr BEC. Th numrical rsults providd in Sction V-B will illustrat this. Finally, not also that, unli th BEC cas, undr BSC th FC nds to now th channl paramtrs {ɛ } to oprat in a channlawar mannr. C. Additiv Whit Gaussian Nois (AWGN Channls Now, assum that th channl btwn ach snsor and th FC is an AWGN channl. Th rcivd signal at th FC is givn by z n = h nx n + w n (14 whr h n = h,, n, is a nown constant complx channl gain; wn N c (0, ; x n is th transmittd signal at sampling tim t n givn by { x a, if λ n = n, b, if λ (15 n. whr th transmission lvls a and b ar complx in gnral. Th distribution of th rcivd signal is thn zn N c (h x n,. Th LLR of z n is givn by λ n = log pa (z np a 1 + p b (z np b 1 p a (z np a 0 + pb (z np b 0 = log (1 β xp( c n + β xp( d n α xp( c n + (1 α xp( d n, (16 whr th suprscript a (rsp. b dnots th conditioning on x n = a (rsp. x n = b, c n z n h a and d n z n h b. D. Rayligh Fading Channls If a Rayligh fading channl is assumd btwn ach snsor and th FC, th rcivd signal modl is also givn by (14-(15, but with h n N c (0, h,. W thn hav zn N c (0, x n h, + ; and accordingly, similar to (16, λ n is writtn as λ n = log 1 β a, xp( c n + β xp( d n b, α xp( c n + 1 α a, xp( d n b, (17 whr a, a h, +, b, b h, +, c n z n a, and d n z n. b, IV. PERFORMANCE ANALYSIS FOR IDEAL CHANNELS In this sction, w driv th xact non-asymptotic xprssion for th avrag dtction dlay E i T, and provid an asymptotic analysis on it as th rror probability bounds α, β 0. Bfor procding to th analysis, lt us dfin som information ntitis which will b usd throughout this and nxt sctions.

4 A. Information Entitis can dfin hypothtical KL information to srv analysis Not that th xpctation of an LLR corrsponds to a purposs. Kullbac-Liblr (KL information ntity. For instanc, Th KL information Ii (1 of a snsor whos information I1 (t E 1 log f 1 (y1,..., yt ratio, η i, is high and clos to 1 is wll projctd to th f0 (y 1,..., = E 1 L y t, FC. Not that thr ar two sourcs of information loss for t snsors, namly, th ovrshoot ffct du to having discrttim obsrvations and noisy transmission channls. Th lattr y t (18 and I0 (t E 0 log f 0 (y1,..., yt f1 (y 1,..., = E 0 L t appars only in η i, whras th formr appars in both ˆη i and η ar th KL divrgncs of th local LLR squnc {L i. In gnral with discrt-tim obsrvations at snsors t } t w hav undr H 1 and H 0, rspctivly. Similarly Îi(1 I i (1 and Ĩi(1 I i (1. Lastly, not that undr idal channls, sinc zn = b n,, n, w hav Î1 (t E 1 log p 1(b 1,..., b Ĩi(1 = Î i (1. Nt p 0 (b 1,..., = E 1 ˆL b t, Î 0 (t E 0 ˆL t B. Analysis on Dtction Dlay Nt Ĩ1 (t E 1 log p 1(z1,..., z Lt {τn : τn = t n t n 1} n dnot th intr-arrival tims Nt p 0 (z 1,..., = E 1 L z t, Ĩ 0 (t E 0 L t of th LLR mssags transmittd from th -th snsor. Not Nt that τn dpnds on th obsrvations y t (19 +1,..., y t and n 1 n, sinc {yt } t ar i.i.d., {τn} n ar also i.i.d. random variabls. ar th KL divrgncs of th local LLR squncs {ˆL t } t and { L t } t rspctivly. Dfin also I i (t Hnc, th counting procss {Nt } t is a rnwal procss. K =1 I i (t, Î i (t K =1 Î i (t, and Ĩi(t Similarly th LLRs {ˆλ n} n of th rcivd signals at th FC K ar also i.i.d. random variabls, and form a rnwal-rward =1 Ĩ i (t as th KL procss. Not from (9 that th SPRT can stop in btwn divrgncs of th global LLR squncs {L t }, {ˆL t }, and two arrival tims of snsor,.g., t { L t } rspctivly. n T < t n+1. Th vnt In particular, w hav I1 (1 = E 1 log f 1 (y 1 N f0 (y 1 = E 1 lt T = n occurs if and only if t n = τ τn T and t and I0 (1 = E 0 log f 0 (y 1 n+1 = τ τn+1 > T, so it dpnds on th first (n+1 f1 (y 1 = E 0 lt as th KL information LLR mssags. From th dfinition of stopping tim 11, pp. numbrs of th LLR squnc {lt 104 w conclud that N }; and I i (1 T is not a stopping tim for th K procsss {τ =1 I i (1, i = 0, 1 ar thos of th global LLR squnc {l t }. Morovr, I1 (t 1 = E 1 n} n and {ˆλ n} n sinc it dpnds on th (n + 1- log f 1 (y 1,...,y t th mssag. Howvr, NT + 1 is a stopping tim for {τ n} n 1 = and {ˆλ f0 (y 1,...,y t n} n sinc w hav NT + 1 = n N T = n 1 1 which dpnds only on th first n LLR mssags. Hnc, E 1 λ n, Î1 (t 1 = E 1 log p 1 (b 1 p 0 (b 1 = E 1 ˆλ n, and Ĩ 1 (t 1 = from Wald s idntity 11, pp. 105 w can dirctly writ th E 1 log p 1 (z 1 p 0 (z 1 = E 1 λ n, ar th KL information numbrs of following qualitis th local LLR squncs {λ n}, {ˆλ n}, and { λ N n}, rspctivly, T +1 undr H 1. Liwis, w hav I0 (t 1 = E 0 λ n, Î0 (t 1 = E i τ n = E i τ1 (E i NT + 1, (0 E 0 ˆλ n, and Ĩ 0 (t 1 = E 0 λ n undr H 0. To summariz, Ii (t, Î i (t, and Ĩ i (t ar rspctivly th obsrvd (at N T +1 snsor, transmittd (by snsor, and rcivd (by th and E i ˆλ n = E i ˆλ 1(E i NT + 1. (1 FC KL information ntitis as illustratd in Fig. 1. Nxt w dfin th following information ratios, ˆη i Î i (t 1 Ii (t 1 and η i Ĩ i (t 1 Ii (t 1, which rprsnt how fficintly information is transmittd from snsor and rcivd by th FC, rspctivly. Du to th data procssing inquality, w hav 0 ˆη i, η i 1, i,. W furthr dfin Î i (1 K =1 ˆη i I i (1 = K =1 Î i (1, and Ĩi(1 K =1 η i I i (1 = K =1 Ĩ i (1, as th ffctiv transmittd and rcivd valus corrsponding to th KL information I i (1, rspctivly. Not that Î i (1 and Ĩi(1 ar not ral KL information numbrs, but projctions of I i (1 onto th filtrations gnratd by th transmittd, (i.., {b n}, and rcivd, (i.., {zn}, signal squncs, rspctivly. This is bcaus snsors do not transmit and th FC dos not rciv th LLR of a singl obsrvation, but instad thy transmit and it rcivs th LLR mssags of svral obsrvations. Hnc, w cannot hav th KL information for singl obsrvations at th two nds of th communication channl, but w W hav th following thorm on th avrag dtction dlay undr idal channls. Thorm 1. Considr th dcntralizd dtction schm givn in Sction II, with idal channls btwn snsors and th FC. Its avrag dtction dlay undr H i is givn by E i T = Îi(T Î i (1 + K =1 Î i (t N T +1 E iy Î i (1 Î i (1 ( whr Y is a random variabl rprsnting th tim intrval btwn th stopping tim and th arrival of th first bit from th -th snsor aftr th stopping tim, i.., Y t N T +1 T. Proof: From (0 and (1 w obtain N N T +1 T E +1 i E i τn = E i τ1 ˆλ n E i ˆλ 1

5 whr th lft-hand sid quals to E i T + E i Y. Not that E i τ1 is th xpctd stopping tim of th local SPRT at th -th snsor and by Wald s idntity it is givn by E i τ1 = E iλ 1 E il1, providd that E il1 0. Hnc, w hav E i T = E iλ 1 E i ˆλ 1 E i N T +1 ˆλ n E i l1 E i Y = I i (t Î 1 i (T + Î i (t N +1 T Îi (t 1 Ii (1 E i Y N T whr w usd th fact that E +1 1 ˆλ n = E 1 ˆL T + Ẽ1ˆλ NT +1 = Î 1 (T + Î 1 (t NT +1 and similarly N T E +1 0 ˆλ n = Î 0 (T Î 0 (t NT +1. Not that Ẽi is th xpctation with rspct to ˆλ NT +1 and N T undr H i. By rarranging th trms and thn summing ovr on both sids, w obtain K E i T I (1Î i (t 1 i I =1 i (t 1 = }{{} Î i(1 Î i (T + K =1 Î i (t N T +1 E iy I i (1Î i (t 1 I i (t 1 }{{} Î i (1 which is quivalnt to (. Th rsult in ( is in fact vry intuitiv. Rcall that Î i (T is th KL information at th dtction tim at th FC. It naturally lacs som local information that has bn accumulatd at snsors, but has not bn transmittd to th FC, i.., th information gathrd at snsors aftr thir last sampling tims. Th numrator of th scond trm on th right hand sid of ( rplacs such missing information by using th hypothtical KL information. Not that in ( Îi (t NT +1 Î i (t 1, i.., Ẽiˆλ NT +1 E iˆλ 1, sinc NT and ˆλ ar not indpndnt. NT +1 Th nxt rsult givs th asymptotic dtction dlay prformanc undr idal channls. Thorm. As α, β 0, th avrag dtction dlay undr idal channls givn by ( satisfis E 1 T = log α Î 1 (1 + O(1, and E log β 0T = Î 0 (1 + O(1, whr O(1 rprsnts a constant trm. (3 Proof: W will prov th first quality in (3, and th proof of th scond on follows similarly. Lt us first prov th following lmma. Lmma 1. As α, β 0 w hav th following KL information at th FC Î 1 (T = log α + O(1, and Î0(T = log β + O(1. (4 Proof: W will show th first quality and th scond on follows similarly. W hav Î 1 (T = P 1 (ˆL T AE 1 ˆL T ˆL T A+ P 1 (ˆL T BE 1 ˆL T ˆL T B = (1 β(a + E 1 θ A β(b + E 1 θ B, (5 whr θ A, θ B ar ovrshoot and undrshoot rspctivly givn by θ A ˆL T A if ˆL T A and θ B ˆL T B if ˆLT B. From 5, Thorm, w hav A log α and B log β, so as α, β 0 (5 bcoms Î 1 (T = A + E 1 θ A + o(1. Assuming 0 < < and lt <,, t, w hav 0 < α, β < 1, hnc from (10 w hav ˆλ n <, and accordingly Î i (t 1 = E i ˆλ 1 <. Sinc th ovrshoot cannot xcd th last rcivd LLR valu, w hav θ A, θ B Θ = max,n ˆλ n <. Similar to Eq. (73 in 5 w can writ β B Θ and α A Θ whr Θ = O(1 by th abov argumnt, or quivalntly, B log β O(1 and A log α O(1. Hnc, w hav A = log α + O(1 and B = log β + O(1. From th assumption of lt <,, t, w also hav Î i (1 I i (1 <. Morovr, w hav E i Y E i τ1 < sinc E i l1 0. Not that all of th trms on th righthand sid of ( xcpt Îi(T do not dpnd on th global rror probabilitis α, β, so thy ar O(1 as α, β 0. Finally, substituting (4 into ( w gt (3. It is sn from (3 that th hypothtical KL information numbr, Î i (1, plays a y rol in th asymptotic dtction dlay xprssion. W can asymptotically minimiz E i T by maximizing Îi(1. Rcalling its dfinition Î i (1 = K =1 Î i (t 1 I i (t 1 I i (1 w s that thr information numbrs ar rquird to comput it. Not that I i (1 = E il 1 and I i (t 1 = E i λ 1, which is givn in (6 blow, ar computd basd on local obsrvations at snsors, thus do not dpnd on th channls btwn snsors and th FC. Spcifically, w hav I 1 (t 1 = (1 β ( + E 1 θ n β ( + E 1 θ n, and I 0 (t 1 = α ( + E 0 θ n (1 α ( + E 0 θ n (6 whr θ n and θ n ar local ovr(undrshoots givn by θ n λ n if λ n and θ n λ n if λ n. Du to having l t <,, t w hav θ n, θ n <,, n. On th othr hand, Î i (t 1 rprsnts th information rcivd in an LLR mssag by th FC, so it havily dpnds on th channl typ. In th idal channl cas, from (10 it is givn by and Î 1 (t 1 = (1 β log 1 β α Î 0 (t 1 = α log 1 β α β + β log, 1 α + (1 α log β 1 α. (7

6 Ĩ 1 (t 1 Sinc Î i (t 1 is th only channl-dpndnt trm in th asymptotic dtction dlay xprssion, in th nxt sction w will obtain its xprssion for ach noisy channl typ considrd in Sction III. V. PERFORMANCE ANALYSIS FOR NOISY CHANNELS In all noisy channl typs that w considr in this papr, w assum that channl paramtrs ar ithr constants or i.i.d. random variabls across tim. In othr words, ɛ, h ar constant for all (s Sction III-A, III-B, III-C, and {h n} n, {w n} n ar i.i.d. for all (s Sction III-C, III-D,??. Thus, in all noisy channl cass discussd in Sction III th intr-arrival tims of th LLR mssags { τ n} n, and th LLRs of th rcivd signals { λ n} n ar i.i.d. across tim as in th idal channl cas. Accordingly th avrag dtction dlay in ths noisy channls has th sam xprssion as in (, as givn by th following proposition. Th proof is similar to that of Thorm 1. Proposition 1. Undr ach typ of noisy channl discussd in Sction III, th avrag dtction dlay is givn by E i T = Ĩi( T K Ĩ i (1 + =1 Ĩ i (t NT +1 EiỸĨ i (1 (8 Ĩ i (1 whr Ỹ t N T +1 T. Th asymptotic prformancs undr noisy channls can also b analyzd analogously to th idal channl cas. Proposition. As α, β 0, th avrag dtction dlay undr noisy channls givn by (8 satisfis E 1 T = log α Ĩ 1 (1 + O(1, and E 0 T log β = Ĩ 0 (1 + O(1. (9 Proof: Not that in th noisy channl cass th FC, as discussd in Sction III, computs th LLR, λ n, of th signal it rcivs, and thn prforms SPRT using th LLR sum L t. Hnc, analogous to Lmma 1 w can show that Ĩ1( T = log α + O(1 and Ĩ0( T = log β + O(1 as α, β 0. Not also that du to channl uncrtaintis λ n ˆλ n, so w hav Ĩ i (t 1 Î i (t 1 < and Ĩi(1 Îi(1 <. W also hav E i Ỹ E i τ 1 < as in th idal channl cas. Substituting ths asymptotic valus in (8 w gt (9. Rcall that Ĩi(1 = K =1 Ĩ i (t 1 I i (t 1 I i (1 in (9 whr I i (1 and I i (t 1 ar indpndnt of th channl typ, i.., thy ar sam as in th idal channl cas. In th subsqunt subsctions, w will comput Ĩ i (t 1 for ach noisy channl typ. W will also considr th choics of th signaling lvls a and b in (15 that maximiz Ĩ i (t 1, i.., asymptotically minimiz E i T. A. BEC Undr BEC, from (11 w can writ th LLR of th rcivd bits at th FC as { ˆλ λ n = n, with probability 1 ɛ, (30 0, with probability ɛ. ǫ α = β Fig.. Th KL information, Ĩ 1 (t 1, undr BEC and BSC, as a function of th local rror probabilitis α = β and th channl rror probability ɛ. Hnc, w hav Ĩ i (t 1 = E i λ 1 = (1 ɛ Î i (t 1 (31 whr Î i (t 1 is givn in (7. As can b sn in (31 th prformanc dgradation undr BEC is only dtrmind by th channl paramtrs ɛ. In gnral, from (3, (9 and (31 this asymptotic prformanc loss can b quantifid as 1 1 min ɛ Ei T 1 E it 1 max ɛ. Spcifically, if ɛ = ɛ,, thn w hav Ei T E it = 1 1 ɛ as α, β 0. B. BSC Rcall from (1 and (13 that undr BSC local rror probabilitis α, β undrgo a linar transformation to yild th ffctiv local rror probabilitis ˆα, ˆβ at th FC. Thrfor, using (1 and (13, similar to (7, Ĩ i (t 1 is writtn as follows and Ĩ 1 (t 1 = (1 ˆβ log 1 ˆβ ˆα Ĩ 0 (t 1 = ˆα log 1 ˆβ ˆα + ˆβ ˆβ log, 1 ˆα (3 ˆβ + (1 ˆα log 1 ˆα whr ˆα = (1 ɛ α + ɛ and ˆβ = (1 ɛ β + ɛ. Notic that th prformanc loss in this cas also dpnds only on th channl paramtr ɛ. In Fig. w plot Ĩ 1 (t 1 as a function of α = β and ɛ, for both BEC and BSC. It is sn that th KL information of BEC is highr than that of BSC, implying that th asymptotic avrag dtction dlay is lowr for BEC, as anticipatd in Sction III-B. C. AWGN In this and th following sctions, w will drop th snsor indx of h, and for simplicity. In th AWGN cas, it follows from Sction III-C that if th transmittd signal is a, i.., x n = a, thn c n = u, d n = v a ; and if x n = b, thn c n = v b, d n = u whr u w n, v a w n +(a bh, v b w n +(b ah. Accordingly, from (16 w writ th KL information as in (33, whr E dnots th xpctation with rspct to th channl nois wn only, and Ē1 dnots th xpctation with rspct to both x n and wn undr H 1.

7 Ĩ1 (t 1 =Ē1 λ 1 = (1 β E log (1 β u + β va α u + β E log (1 β v b + β u + (1 α va α v b + (1 α u { }}{ = (1 β log 1 β β ( 1 β + β log +β E log 1 + β { }}{ 1 β u va α 1 α }{{ β } α + E log β β u v b α u va 1 + α 1 α u v b }{{} Î1 (t 1 C1 E 1 E (33 Sinc wn is indpndnt of x n undr both H 0 and H 1, w usd th idntity Ē1 = EE 1 in (33. Not from (33 that w hav Ĩ 1 (t 1 = Î 1 (t 1 + β C1 and Ĩ 0 (t 1 = Î 0 (t 1 + α C0. Similar to C1 w hav C0 E 1 1 α α E. Sinc w now Ĩ i (t 1 Î i (t 1, th xtra trms, C1, C0 0 ar pnalty trms that corrspond to th information loss du to th channl nois. Our focus will b on this trm as w want to optimiz th prformanc undr AWGN channls by choosing th transmission signal lvls a and b that maximiz Ci. Lt us first considr th random variabls ζ a u v a and ζ b u v b which ar th argumnts of th xponntial functions in E 1 and E in (33. From th dfinitions of u and v a, w writ ζ a = w n w n +(a bh = a b h γ whr γ R{(wn (a bh } and R{ } dnots th ral part of a complx numbr. Similarly w hav ζ b = a b h + γ. Not that γ N (0, a b h sinc wn N c (0,. If w dfin ν a b h γ, thn w hav ν N (0, 1. Upon dfining s a b h w can thn writ ζ a and ζ b as ζ a = s sν and ζ b = s + sν. If w dfin F 1 α α C0 =E C 1 =E log 1 + F 1 ζ b 1 + G ζ b log 1 + Gζ b 1 + F 1 ζ b and G 1 β β, thn w hav + F 1 E log 1 + F ζa + GE 1 + G 1 ζa log 1 + G 1 ζa. 1 + F ζa (34 Not from (14 that th rcivd signal, z n, will hav th sam varianc, but diffrnt mans, ah and bh, if x n = a and x n = b ar transmittd rspctivly. Hnc, w xpct that th dtction prformanc undr AWGN channls will improv if th diffrnc btwn th transmission lvls, a b, incrass. Toward that nd th following rsult givs a sufficint condition undr which th pnalty trm C i incrass with s, and hnc with a b. Th proof is givn in 10, Appndix. Lmma. Ci is an incrasing function of s, i = 0, 1, if F G and G F. Lmma indicats that for α, β valus insid th rgion shown in Fig. 3, Ci is incrasing in a b. Not that α, β ar local rror probabilitis which ar dirctly rlatd to th local thrshold. Thrfor, vn if th hypothss H 0 and H 1 ar non-symmtric, w can nsur that w will hav β α Fig. 3. Th rgion of (α, β spcifid by Lmma. α, β insid th rgion in Fig. 3 by mploying diffrnt local thrsholds, and, in (. In fact, vn for α, β valus outsid th rgion in Fig. 3 numrical rsults show that Ci is incrasing in s. Hnc, maximizing Ci is quivalnt to maximizing a b. If w considr a constraint on th maximum allowd transmission powr at snsors, i.., max( a, b P, thn th antipodal signaling is optimum, i.., a = b = P and a = b. D. Rayligh Fading It follows from Sction III-D that c n = u a, d n = a u b a whn x n = a; and c n = b u a b, d n = u b whn x n = b whr u a ah n +w n, u a b bh n +w n, and b a = a h +, b = b h + as dfind in Sction III-D. Dfin furthr ρ a. Hnc, using (17 w writ th KL information as in b (35, whr ζ a u a (1 ρ and ζ b u b (1 ρ 1. Not that whn a = b which corrsponds to th optimal signaling in th AWGN cas, w hav ρ = 1, ζ a = ζ b = 0 and thrfor Ĩ1 (t 1 = 0 in (35. This rsult is quit intuitiv sinc in th Rayligh fading cas th rcivd signals diffr only in thir variancs. Not that u a and u b ar chi-squard random variabls with dgrs of frdom, i.., u a, u b χ, thus w can writ th pnalty trm Ci as C 0 = 0 ( log 1 + F 1 ρ 1 u(1 ρ Gρ 1 u(1 ρ 1 F 1 log 1 + F ρu(1 ρ 1 + G 1 ρ u(1 ρ u du, (36

8 1 β a ua + β b ρua 1 β a ρ 1 u b + β u b b Ĩ1 (t 1 =(1 β E log α a ua + 1 α + β E log b ρua α a ρ 1 u b + 1 α u b b = (1 β log 1 β β + β log +β (E log 1 + Gρ 1 ζ b α 1 α }{{ 1 + F } 1 ρ 1 ζ + GE log 1 + G 1 ρ ζa b 1 + F ρ }{{ ζa } Î1 (t 1 C1 (35 Rayligh Fading btwn H 0 and H 1 around ρ = 1 will xist whnvr F = G, i.., α = β. C i Fig. 4. Th pnalty trm Ci for Rayligh fading channls as a function of ρ. and C 1 = 0 ( log 1 + Gρ 1 u(1 ρ F 1 ρ 1 u(1 ρ 1 + ρ G log 1 + G 1 ρ u(1 ρ 1 + F ρ u(1 ρ H1 H 0 u du. (37 Not that givn local rror probabilitis α, β th intgrals in (36, (37 is a function of ρ only. Howvr, maximizing Ci in (36, (37 with rspct to ρ sms analytically intractabl. As can b sn in Sction III-D, th rcivd signals at th FC will hav zro man and th variancs a and b whn x n = a and x n = b rspctivly. Thrfor, in this cas intuitivly w should incras th diffrnc btwn th two variancs, i.., a b. Considr th following constraints: max( a, b P and min( a, b Q, whr th first on is th pa powr constraint as bfor, and th scond is to nsur rliabl dtction of an incoming signal by th FC. W conjctur that th optimum signaling schm in this cas that maximizs Ci corrsponds to a = P, b = Q or a = Q, b = P. To numrically illustrat th bhavior of Ci as a function of ρ, w st α = β = 0.1, h = = 1, P = 10, Q = 1, and plot Ci in Fig. 4. It is sn that Ci has its global minimum whn ρ = 1, which corrsponds to th cas a = b as xpctd. Morovr, Ci, validating our conjctur, monotonically grows as ρ tnds to its minimum and maximum valus corrsponding to th cass a = Q, b = P and a = P, b = Q rspctivly. Not that in Fig. 4, th curvs for H 0 and H 1 ar mirrord vrsions of ach othr around ρ = 1 sinc w hav α = β in th xampl. From (36, (37 w can say that th symmtry VI. CONCLUSIONS W hav dvlopd and analyzd channl-awar distributd dtction schms basd on lvl-triggrd sampling. Th snsors form local log-lilihood ratios (LLRs basd on thir obsrvations and sampl thir LLRs using th lvl-triggrd sampling. Upon sampling ach snsor snds a singl bit to th fusion cntr (FC. Th FC is quippd with th local rror rats of all snsors and th statistics of th channls from all snsors. Upon rciving th bits from th snsors, th FC updats th global LLR and prforms an SPRT. Th fusion ruls undr diffrnt channl typs ar givn. W hav furthr providd non-asymptotic and asymptotic analyss on th avrag dtction dlay for th proposd channl-awar schm. W hav shown that th asymptotic dtction dlay is charactrizd by a KL information numbr, whos xprssions undr diffrnt channl typs hav bn drivd. Basd on th dlay analysis, w hav also idntifid appropriat signaling schms undr diffrnt channls for th snsors to transmit th 1-bit information. REFERENCES 1 R.R. Tnny, and N.R. Sandll, Dtction with distributd snsors, IEEE Trans. Aro. Elctron. Syst., vol. 17, no. 4, pp , July Z. Chair, and P.K. Varshny, Optimal data fusion in multipl snsor dtction systms, IEEE Trans. Aro. Elctron. Syst., vol., no. 1, pp , Jan V.V. Vravalli, T. Basar, and H.V. Poor, Dcntralizd squntial dtction with a fusion cntr prforming th squntial tst, IEEE Trans. Inform. Thory, vol. 39, no., pp , Mar Y. Mi, Asymptotic optimality thory for squntial hypothsis tsting in snsor ntwors, IEEE Trans. Inform. Thory, vol. 54, no. 5, pp , May G. Fllouris, and G.V. Moustaids, Dcntralizd squntial hypothsis tsting using asynchronous communication, IEEE Trans. Inform. Thory, vol. 57, no. 1, pp , Jan Y. Yilmaz, G.V. Moustaids, and X. Wang, Cooprativ squntial spctrum snsing basd on lvl-triggrd sampling, IEEE Trans. Sig. Proc., vol. 60, no. 9, pp , Sp V. Poor, An Introduction to Signal Dtction and Estimation, Springr, Nw Yor, NY, B. Chn, L. Tong and P.K. Varshny, Channl-Awar Distributd Dtction in Wirlss Snsor Ntwors, IEEE Signal Procssing Magazin, vol. 3, issu 4, pp. 16-6, July A. Wald and J. Wolfowitz, Optimum charactr of th squntial probability ratio tst, Ann. Math. Stat., vol. 19, pp , Y. Yilmaz, G.V. Moustaids, and X. Wang, Channlawar Dcntralizd Dtction via Lvl-triggrd Sampling, Sp S. Ross, Stochastic Procsss, Wily, Nw Yor, NY, 1996.

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

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

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

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

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

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

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

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.

Probability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J. Probability and Stochastic Procsss: A Frindly Introduction for Elctrical and Computr Enginrs Roy D. Yats and David J. Goodman Problm Solutions : Yats and Goodman,4.3. 4.3.4 4.3. 4.4. 4.4.4 4.4.6 4.. 4..7

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

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM

LINEAR DELAY DIFFERENTIAL EQUATION WITH A POSITIVE AND A NEGATIVE TERM Elctronic Journal of Diffrntial Equations, Vol. 2003(2003), No. 92, pp. 1 6. ISSN: 1072-6691. URL: http://jd.math.swt.du or http://jd.math.unt.du ftp jd.math.swt.du (login: ftp) LINEAR DELAY DIFFERENTIAL

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

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

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES. 1. Statement of results

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES. 1. Statement of results BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim and n a positiv intgr, lt ν p (n dnot th xponnt of p in n, and u p (n n/p νp(n th unit part of n. If α

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

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

(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

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

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

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

Elements of Statistical Thermodynamics

Elements of Statistical Thermodynamics 24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,

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

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

1 Minimum Cut Problem

1 Minimum Cut Problem CS 6 Lctur 6 Min Cut and argr s Algorithm Scribs: Png Hui How (05), Virginia Dat: May 4, 06 Minimum Cut Problm Today, w introduc th minimum cut problm. This problm has many motivations, on of which coms

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

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers: APPM 6 Final 5 pts) Spring 4. 6 pts total) Th following parts ar not rlatd, justify your answrs: a) Considr th curv rprsntd by th paramtric quations, t and y t + for t. i) 6 pts) Writ down th corrsponding

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

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

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

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

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

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES

BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES BINOMIAL COEFFICIENTS INVOLVING INFINITE POWERS OF PRIMES DONALD M. DAVIS Abstract. If p is a prim (implicit in notation and n a positiv intgr, lt ν(n dnot th xponnt of p in n, and U(n n/p ν(n, th unit

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

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

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018 Propositional Logic Combinatorial Problm Solving (CPS) Albrt Olivras Enric Rodríguz-Carbonll May 17, 2018 Ovrviw of th sssion Dfinition of Propositional Logic Gnral Concpts in Logic Rduction to SAT CNFs

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

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

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

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

Continuous probability distributions

Continuous probability distributions Continuous probability distributions Many continuous probability distributions, including: Uniform Normal Gamma Eponntial Chi-Squard Lognormal Wibull EGR 5 Ch. 6 Uniform distribution Simplst charactrizd

More information

Asymptotically Optimal and Bandwith-efficient Decentralized Detection

Asymptotically Optimal and Bandwith-efficient Decentralized Detection Asymptotically Optimal and Bandwith-efficient Decentralized Detection Yasin Yılmaz and Xiaodong Wang Electrical Engineering Department, Columbia University New Yor, NY 10027 Email: yasin,wangx@ee.columbia.edu

More information

Equidistribution and Weyl s criterion

Equidistribution and Weyl s criterion Euidistribution and Wyl s critrion by Brad Hannigan-Daly W introduc th ida of a sunc of numbrs bing uidistributd (mod ), and w stat and prov a thorm of Hrmann Wyl which charactrizs such suncs. W also discuss

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

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

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

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

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

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

On the irreducibility of some polynomials in two variables

On the irreducibility of some polynomials in two variables ACTA ARITHMETICA LXXXII.3 (1997) On th irrducibility of som polynomials in two variabls by B. Brindza and Á. Pintér (Dbrcn) To th mmory of Paul Erdős Lt f(x) and g(y ) b polynomials with intgral cofficints

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

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

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

General Notes About 2007 AP Physics Scoring Guidelines

General Notes About 2007 AP Physics Scoring Guidelines AP PHYSICS C: ELECTRICITY AND MAGNETISM 2007 SCORING GUIDELINES Gnral Nots About 2007 AP Physics Scoring Guidlins 1. Th solutions contain th most common mthod of solving th fr-rspons qustions and th allocation

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

Brief Introduction to Statistical Mechanics

Brief Introduction to Statistical Mechanics Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.

More information

CS 361 Meeting 12 10/3/18

CS 361 Meeting 12 10/3/18 CS 36 Mting 2 /3/8 Announcmnts. Homwork 4 is du Friday. If Friday is Mountain Day, homwork should b turnd in at my offic or th dpartmnt offic bfor 4. 2. Homwork 5 will b availabl ovr th wknd. 3. Our midtrm

More information

Content Based Status Updates

Content Based Status Updates Contnt Basd Status Updats li Najm LTHI, PFL, Lausann, Switzrland mail: li.najm@pfl.ch Rajai Nassr LTHI, PFL, Lausann, Switzrland mail: rajai.nassr@pfl.ch mr Tlatar LTHI, PFL, Lausann, Switzrland mail:

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

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon.

4. Money cannot be neutral in the short-run the neutrality of money is exclusively a medium run phenomenon. PART I TRUE/FALSE/UNCERTAIN (5 points ach) 1. Lik xpansionary montary policy, xpansionary fiscal policy rturns output in th mdium run to its natural lvl, and incrass prics. Thrfor, fiscal policy is also

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

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

3-2-1 ANN Architecture

3-2-1 ANN Architecture ARTIFICIAL NEURAL NETWORKS (ANNs) Profssor Tom Fomby Dpartmnt of Economics Soutrn Mtodist Univrsity Marc 008 Artificial Nural Ntworks (raftr ANNs) can b usd for itr prdiction or classification problms.

More information

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction

A Prey-Predator Model with an Alternative Food for the Predator, Harvesting of Both the Species and with A Gestation Period for Interaction Int. J. Opn Problms Compt. Math., Vol., o., Jun 008 A Pry-Prdator Modl with an Altrnativ Food for th Prdator, Harvsting of Both th Spcis and with A Gstation Priod for Intraction K. L. arayan and. CH. P.

More information

Using Stochastic Approximation Methods to Compute Optimal Base-Stock Levels in Inventory Control Problems

Using Stochastic Approximation Methods to Compute Optimal Base-Stock Levels in Inventory Control Problems Using Stochastic Approximation Mthods to Comput Optimal Bas-Stoc Lvls in Invntory Control Problms Sumit Kunnumal School of Oprations Rsarch and Information Enginring, Cornll Univrsity, Ithaca, Nw Yor 14853,

More information

Cramér-Rao Inequality: Let f(x; θ) be a probability density function with continuous parameter

Cramér-Rao Inequality: Let f(x; θ) be a probability density function with continuous parameter WHEN THE CRAMÉR-RAO INEQUALITY PROVIDES NO INFORMATION STEVEN J. MILLER Abstract. W invstigat a on-paramtr family of probability dnsitis (rlatd to th Parto distribution, which dscribs many natural phnomna)

More information

Thus, because if either [G : H] or [H : K] is infinite, then [G : K] is infinite, then [G : K] = [G : H][H : K] for all infinite cases.

Thus, because if either [G : H] or [H : K] is infinite, then [G : K] is infinite, then [G : K] = [G : H][H : K] for all infinite cases. Homwork 5 M 373K Solutions Mark Lindbrg and Travis Schdlr 1. Prov that th ring Z/mZ (for m 0) is a fild if and only if m is prim. ( ) Proof by Contrapositiv: Hr, thr ar thr cass for m not prim. m 0: Whn

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

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM

COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM COUNTING TAMELY RAMIFIED EXTENSIONS OF LOCAL FIELDS UP TO ISOMORPHISM Jim Brown Dpartmnt of Mathmatical Scincs, Clmson Univrsity, Clmson, SC 9634, USA jimlb@g.clmson.du Robrt Cass Dpartmnt of Mathmatics,

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

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

Chapter 13 Aggregate Supply

Chapter 13 Aggregate Supply Chaptr 13 Aggrgat Supply 0 1 Larning Objctivs thr modls of aggrgat supply in which output dpnds positivly on th pric lvl in th short run th short-run tradoff btwn inflation and unmploymnt known as th Phillips

More information

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1 Chaptr 11 Th singular sris Rcall that by Thorms 10 and 104 togthr provid us th stimat 9 4 n 2 111 Rn = SnΓ 2 + on2, whr th singular sris Sn was dfind in Chaptr 10 as Sn = q=1 Sq q 9, with Sq = 1 a q gcda,q=1

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

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

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

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

Observer Bias and Reliability By Xunchi Pu

Observer Bias and Reliability By Xunchi Pu Obsrvr Bias and Rliability By Xunchi Pu Introduction Clarly all masurmnts or obsrvations nd to b mad as accuratly as possibl and invstigators nd to pay carful attntion to chcking th rliability of thir

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

On spanning trees and cycles of multicolored point sets with few intersections

On spanning trees and cycles of multicolored point sets with few intersections On spanning trs and cycls of multicolord point sts with fw intrsctions M. Kano, C. Mrino, and J. Urrutia April, 00 Abstract Lt P 1,..., P k b a collction of disjoint point sts in R in gnral position. W

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

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

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

Deift/Zhou Steepest descent, Part I

Deift/Zhou Steepest descent, Part I Lctur 9 Dift/Zhou Stpst dscnt, Part I W now focus on th cas of orthogonal polynomials for th wight w(x) = NV (x), V (x) = t x2 2 + x4 4. Sinc th wight dpnds on th paramtr N N w will writ π n,n, a n,n,

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

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

UNTYPED LAMBDA CALCULUS (II)

UNTYPED LAMBDA CALCULUS (II) 1 UNTYPED LAMBDA CALCULUS (II) RECALL: CALL-BY-VALUE O.S. Basic rul Sarch ruls: (\x.) v [v/x] 1 1 1 1 v v CALL-BY-VALUE EVALUATION EXAMPLE (\x. x x) (\y. y) x x [\y. y / x] = (\y. y) (\y. y) y [\y. y /

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

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

Least Favorable Distributions to Facilitate the Design of Detection Systems with Sensors at Deterministic Locations

Least Favorable Distributions to Facilitate the Design of Detection Systems with Sensors at Deterministic Locations Last Favorabl Distributions to Facilitat th Dsign o Dtction Systms with Snsors at Dtrministic Locations Bndito J. B. Fonsca Jr. Sptmbr 204 2 Motivation Rgion o intrst (city, park, stadium 3 Motivation

More information

Mutually Independent Hamiltonian Cycles of Pancake Networks

Mutually Independent Hamiltonian Cycles of Pancake Networks Mutually Indpndnt Hamiltonian Cycls of Pancak Ntworks Chng-Kuan Lin Dpartmnt of Mathmatics National Cntral Univrsity, Chung-Li, Taiwan 00, R O C discipl@ms0urlcomtw Hua-Min Huang Dpartmnt of Mathmatics

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

First derivative analysis

First derivative analysis Robrto s Nots on Dirntial Calculus Chaptr 8: Graphical analysis Sction First drivativ analysis What you nd to know alrady: How to us drivativs to idntiy th critical valus o a unction and its trm points

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

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

P. Bruschi - Notes on Mixed Signal Design

P. Bruschi - Notes on Mixed Signal Design Chaptr 1. Concpts and dfinitions about Data Acquisition Systms Elctronic systms An lctronic systms is a complx lctronic ntwor, which intracts with th physical world through snsors (input dvics) and actuators

More information

MATH 1080 Test 2-SOLUTIONS Spring

MATH 1080 Test 2-SOLUTIONS Spring MATH Tst -SOLUTIONS Spring 5. Considr th curv dfind by x = ln( 3y + 7) on th intrval y. a. (5 points) St up but do not simplify or valuat an intgral rprsnting th lngth of th curv on th givn intrval. =

More information

Finding low cost TSP and 2-matching solutions using certain half integer subtour vertices

Finding low cost TSP and 2-matching solutions using certain half integer subtour vertices Finding low cost TSP and 2-matching solutions using crtain half intgr subtour vrtics Sylvia Boyd and Robrt Carr Novmbr 996 Introduction Givn th complt graph K n = (V, E) on n nods with dg costs c R E,

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

Mor Tutorial at www.dumblittldoctor.com Work th problms without a calculator, but us a calculator to chck rsults. And try diffrntiating your answrs in part III as a usful chck. I. Applications of Intgration

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

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