Capacity of MIMO Channels with Antenna Selection

Size: px
Start display at page:

Download "Capacity of MIMO Channels with Antenna Selection"

Transcription

1 1 Capaity of MIMO Channels with Antenna Seletion Shahab Sanayei and Aria Nosratinia Department of Eletrial Engineering The University of Texas at Dallas, Rihardson, TX Abstrat We explore the apaity of MIMO hannels in the presene of antenna seletion. Antenna seletion redues the omplexity of the radio devies and requires only a small amount of hannel state feedbak to the transmit side. For high SNR, we define the apaity gain as the onstant term in the expansion of the ergodi apaity in terms of SNR. We show that this value is representative of the hannel state information (CSI) at the transmitter. We investigate the asymptoti behavior of the apaity gain for three ases: omplete CSI, no CSI, and partial CSI at transmitter (antenna seletion). We show that while water-filling provides a apaity gain that inreases logarithmially in M (the number of transmit antennas), the apaity gain of transmit antenna seletion behaves only like log(log M). For the low SNR ase, we use the onept of hannel gain, a measure introdued by Verdu [1. We show that hannel gain for antenna seletion inreases only logarithmially in M as opposed to water-filling hannel gain whih inreases linearly in M. The methodology developed in this paper, although motivated by antenna seletion, is fairly general and is useful whenever partial CSI is available at the transmitter. The same tehniques are also applied to the reeive seletion, and orresponding results are noted in hight- and low-snr regimes. I. INTRODUCTION In MIMO systems, the ost and omplexity of multiple RF-hains, power amplifiers, and low noise amplifiers (LNA) is a serious pratial issue. One solution to the ost/omplexity problem is antenna subset seletion [2, [3, [4, [5. At the reeive side, antenna subset seletion redues the omplexity. At the transmit side, antenna subset seletion not only redues the omplexity, but also improves the apaity of the MIMO system [6, [7,

2 2 [8, [9 at the ost of a minimal amount of feedbak. Fast and effiient algorithms have been devised to determine the seleted antenna subsets [10, [11, [12. However, despite the pratial importane of antenna seletion, the information theoreti properties of the resulting hannels remains a mostly unexplored territory. A few notable exeptions exist [13, [14, however, to date losed form expressions for apaity have not been available. In this paper, we analyze the apaity of the antenna seletion hannel in the high-snr and low-snr regimes. In the high-snr regime, we define the notion of apaity gain as the onstant term in the high- SNR expansion of the apaity expression, and demonstrate that it is diretly related to transmit-side hannel state information. This onept was first introdued in [8, [9 and is losely related to a similar onept that was independently proposed by Lozano et al. [15. We are able to draw onlusions about the behavior of the system in the asymptote of large number of transmit antennas, and draw omparisons between the antenna seletion apaity and water-filling apaity. Our results have interesting impliations in the design and analysis of all MIMO systems (not just antenna seletion). The waterfilling apaity (C wf ) has the same growth rate as the apaity of the uninformed transmitter (C) [16, but nevertheless C wf > C with non-vanishing differene at high SNR 1. The differene is an exess rate that is due to hannel state feedbak. The exess rate is not limited to waterfilling; when partial CSI is available at the transmitter the exess rate is still there, but is smaller. Examples of partial CSI inlude transmit antenna seletion and hannel ovariane feedbak. The growth of this exess rate with the number of transmit antennas is a measure of how effetively CSI is being used by a given method. The above developments, the reader may reall, were in the high-snr regime. In the low-snr regime we employ a similar methodology for analysis. In partiular, we look at the power series expansion of the apaity around SNR=0, where the oeffiient of the first-order term is alled hannel gain 2, a quantity that is related to the hannel state information. Using this notion, we show that at low SNR, the optimal seletion strategy at the transmitter is to selet exatly one transmit antenna, regardless of other parameters. This is ew result that is reminisent of, but distint from, the well-known water-filling result at low SNR. Finally, motivated by the symmetry inherent in the problem, we analyze the reeive side antenna seletion in a manner similar to transmit seletion. Even if no multiplexing is lost due to seletion, 1 We assume there are more transmit than reeive antennas. 2 Terminology due to Verdu [1

3 3 reeive antenna seletion inurs a loss of reieve power due to de-seleted antennas, thus, unlike transmit seletion whih may inrease apaity (under onditions mentioned earlier), reeive seletion always inurs a apaity loss. In eah of the low- and high-snr regimes, we fous on three important ases: full CSI at transmitter, no CSI at transmitter, and antenna-seletion CSI at transmitter. In the latter ase, apaity analysis naturally depends on the antenna seletion algorithm. Optimal antenna seletion is not only pratially diffiult, it also indues hannel distributions that do not lead to a tratable formulation. Thankfully there exist antenna seletion algorithms that deliver apaities almost indistinguishable from optimal seletion [11, [8. In this paper we undertake the analysis of antenna seletion using these algorithms. We use the following notation. E[ refers to expeted value of a random variable, I N denotes the N N identity matrix, (x) + = max{x, 0}, and γ is the Euler-Masheroni onstant. We use = bn to denote the asymptoti equivalene of and defined as: lim n bn = 1. We use the natural logarithm throughout this paper so the apaity unit is in Nats/Se/Hz. The hi-square distribution with 2p degrees of freedom is shown by χ 2 2p, and the maximum of n independent χ2 2p distributions is denoted by χ 2 2p,n. With an abuse of notation, we show random variables following the latter distribution also with χ 2 2p,n. II. SYSTEM MODEL We assume a frequeny non-seletive (flat) linear time invariant fading hannel between M transmit and N reeive antennas. The signal model is: y(t) = Hx(t) + n(t) (1) where y(t) represents the N 1 reeived vetor sampled at time t, and x(t) represents the M 1 vetor transmitted by the antennas with power onstrain E[x H x ρ, where ρ is the average SNR (per hannel use), n(t) is the N 1 additive irularly symmetri omplex Gaussian noise vetor with zero mean and ovariane matrix equal to I N (the N N identity matrix) and H is the N M hannel matrix, whose ij-th element is the salar hannel between the i-th reeive and j-th transmit antenna. We assume that the elements of H are independent and have omplex Gaussian distribution with zero mean and unit variane. We also assume that H is perfetly known at the reeiver but it is not neessarily known at the transmitter. For antenna seletion, we assume there is a rate-limited feedbak hannel from reeiver to transmitter so that a subset of transmit antennas an be seleted by the reeiver and furthermore we assume that the feedbak hannel is without error or delay.

4 4 1) Let S 1 = {all olumns of H} and P 1 = I N. 2) hoose h 1 = arg max h S1 h 2, H1 = h 1. 3) for i = 2 : L a) S i = S i 1 { h i 1 } b) Pi = I ρ H L i 1 (I + ρ H L i 1 H H i 1 ) 1 HH i 1 ) h i = arg max h Si h H Pi h d) Hi = [ H i 1 hi 4) H = HL Fig. 1. Antenna seletion algorithm III. TRANSMIT ANTENNA SELECTION We onsider a transmit antenna seletion sheme where a subset of transmit antennas are used for transmission with equal power. Optimal transmit antenna seletion via exhaustive searh among all M L ombinations has omplexity O(M L ), whih is impratial for large number of transmit antennas. One may redue this omplexity by employing a suessive seletion sheme, i.e., a greedy algorithm that at eah step maximizes the apaity of the seleted sub-hannel. A very similar methodology was mentioned in [10 for reeive antenna seletion. In this work, starting from the original hannel matrix, the algorithm removes antennas one after another in a way that the apaity loss is minimized. Gharavi-Alkhansari and Greshman [12 showed that an inremental suessive seletion leads to less omputational omplexity. Simulation results show that this suessive seletion aptures almost all the apaity of optimal antenna seletion in a wide range of SNRs. Therefore, we adopt the latter algorithm for our analysis. The input of the algorithm onsists of ρ (the given SNR), L (the desired number of transmit antennas to be seleted) and H (the original hannel matrix). The output of the algorithm is H (the hannel matrix assoiated with seleted transmit antennas). This algorithm, shown in Figure 1, is the basis for the following analysis.

5 5 A. A Framework for High SNR Analysis Using the Sherman-Morisson formula for determinants [17, for the seleted hannel H we have: det(i N + ρ L H H L H ) = (1 + L h ρ H i P i hi ) (2) As ρ, P i P i, where, P i = I N H i 1 ( H H i 1 H i 1 ) 1 Hi 1 is a projetion matrix of rank N i+1. When M is also large, at eah seletion step, the distribution of the remaining hannel vetors an still be well approximated by a irularly symmetri Gaussian distribution. Our simulations verify that for large M the Gaussianity assumption provides a good approximation for the atual distribution of the remaining olumns. 3 Using this assumption we an approximate the statistis of the right side of (2). We know that for an unorrelated omplex Gaussian vetor x and a projetion matrix P, x H P x has χ 2 distribution with rank(p ) degrees of freedom. Hene for large ρ and large M, we have: det( H H H ) L χ 2 2(N i+1),m i+1 (3) where χ 2 2p,n stands for a random variable whih is the maximum of n independent χ2 2p random variables. The pdf of this random variable an be omputed in losed form [18: where e p (x) = p 1 k=0 xk k!. f χ 2 2p,n (x) = nxp 1 (p 1)! e x (1 e x e p (x)) n 1 (4) B. Capaity gain of MIMO systems We introdue the onept of apaity gain as a measure of effetiveness of hannel state information at the transmitter. We start with the apaity expression for a general MIMO system. Under the flat fading assumption, given a general hannel matrix, the ergodi apaity of the MIMO hannel is alulated as follows [19: C = E[ max tr(q) ρ log(det(i N + HQH H )) (5) where Q = E[xx H is the ovariane of the transmitted vetor x. We onsider three different ases: First, uninformed transmission in whih CSI is perfetly known at reeiver, but not at transmitter. Seond, informed transmission in whih CSI is perfetly known both at transmitter and reeiver. Third, transmission using an optimal subset of transmit antennas seleted by the reeiver. The only information 3 We have no formal proof for this, however, and even for very simple ases it is an open problem and there is no known analytial result.

6 G wf 12 G as Spetral effiieny Bits/se/Hz m log(ρ) 2 No Tx Ant. Sel. (optimal) Ant. Sel. (suessive) Water filling SNR (db) Fig. 2. Capaity gain of antenna seletion: M=8 N=L=2 available at the transmitter is the indies of the seleted transmit antennas. Figure 2 shows the ergodi apaity and the apaity gain for the above three ases. Uninformed transmitter: As shown in [19, when CSI is available only at the reeiver, the ovariane matrix that maximizes the apaity is of the form Q = 1 M I N, hene, the ergodi apaity is: [ C = E[log(det(I N + ρ m M HHH )) = E log(1 + ρ M λ i) where where λ 1,..., λ m are ordered nonzero eigenvalues of the Wishart matrix HH H [19, and m = rank(h) = min{m, N} is the degrees of freedom of the MIMO hannel, assuming hannel is full-rank. As shown in [20, C = m log ρ + O(1). So the ergodi apaity grows linearly with m. Now we notie that in the asymptoti expansion of C there is a onstant term that does not vanish as ρ. Thus we define the apaity gain as follows: For uninformed transmission we have: G = lim (C m log ρ) (6) ρ

7 7 ( [ m ) G = lim E log(1 + ρ ρ M λ i) m log ρ [ m = lim E log( 1 ρ ρ + λ i M ) [ m = E log λ i m log M (7) in the last step, the exhange of expetation and limit is allowed by the monotone onvergene theorem. Informed transmitter (water-filling apaity): In this ase the hannel state information is available at transmitter. As addressed in [19 the water-filling apaity of the MIMO hannel is: [ m C wf = E (log(µλ i )) + where µ should satisfy ρ = m (µ λ 1 i ) +. In large SNR senario, all the eigenmodes of the hannel are used by the beamformer, hene µ = ρ+ m λ 1 i m and the water-filling apaity is equal to: [ m C wf = E (log(µλ i )) = me [ log(ρ + [ m m λ 1 i ) + E log λ i m log m (9) For large ρ we have: C wf m log ρ. In other words, availability of CSI at transmitter side has no impat on the logarithmi growth rate of the ergodi apaity, beause the growth rate only depends on the rank of the hannel matrix. Now we similarly alulate the apaity gain for informed transmission: [ m G wf = E log λ i m log m (10) (8) G = G wf G = m log(m/m) (11) In the asymptote of large SNR, this is the maximum amount of exess rate obtainable by providing hannel state information at the transmitter. We note that if M N then G = 0, thus hannel state information at transmitter annot provide any exess rate asymptotially. This result agrees with one s intuition that beamforming is effetive only when the number of transmit antennas is large. In the sequel, we only onsider the interesting ase of M > N. In partiular, we are interested to understand the behavior of the apaity gain when M N. In these ases, Equation (11) suggests that at high SNR, the

8 8 apaity gain an be used as an information-theoreti metri to evaluate any method that uses hannel state information at the transmitter. Antenna seletion: In the high SNR regime, one is interested in the ase L N, to maintain the degrees of freedom of the hannel and prevent exessive rate loss. Suppose we have seleted L (L N) out of M transmit antennas (M N) then if the seleted hannel is H, the apaity gain is: [ ( G = lim E log det(i N + ρ ρ L H H ) H ) N log ρ [ ( = lim log det( 1 ρ I N + 1 ) L H H H ) = E ρ E [ ( log det( H H ) H ) N log L (12) IV. ASYMPTOTIC BEHAVIOR OF CAPACITY GAIN In this setion we explore the behavior of apaity gain, for large M, in the ase of informed, uninformed, and antenna seletion transmitter. Uninformed transmitter: in the ase M > N, Equation (7) an be rewritten as: G = E [ log det(hh H ) N log M (13) It is known [20 that det(hh H ) N χ2 2(M i+1) therefore [21: where ψ(n) = γ + n 1 k=1 1 k G = N (ψ(m i + 1) log M) (14) is the di-gamma funtion. We have [20: lim G = 0 (15) M Informed transmitter: Using Equations (11) and (15) for large M we have: G wf = N log( M N ) = N log M (16) Antenna seletion: Using the results of Setion III-A, we an evaluate the apaity gain for antenna seletion. Using (12): [ G = E log det( H H H ) N log L = L E[log( χ 2 2(N i+1),m i+1 ) N log L (17)

9 9 Equation (17) suggests that for large M, seleting more than N antennas does not provide any further gain. In the previous setion we argued that L annot be less than N, hene for large M the optimal value for L is N. Heneforth we assume L = N. To evaluate the asymptoti behavior of G, we only need to evaluate E[log X, where X χ 2 p,n. We use the following result from order statistis [18: Definition 1: A df F is said to belong to the domain of maximal attration of ondegenerate df U if there exist sequenes { } and { > 0} suh that at all ontinuity points of U(x). lim F n ( + x) = U(x) (18) n Theorem 1: Let X (n) be the maximum of n i.i.d. random variables {X i } n, eah with df F. If F belongs to the domain of maximal attration of U, then: X (n) d W (19) where W is a random variable whose df is U. Moreover U an only be one of the following three distributions: U 1 (x) = exp( e x ) < x <, exp( x α ) x > 0, α > 0 U 2 (x) =, 0 x 0 1 x > 0 U 3 (x) =, exp( ( x) α ) x 0, α > 0 these distributions are also known as Gumbel, Fréhet and Weilbull distributions, repetively. Theorem 1 is analogue to the entral limit theorem whih was for the normalized sum of iid random variables. Although unlink the entral limit theorem, the normaliziation ontrants and are not neessarily unique. One way to find onstant is to solve the following equation [18: = F 1 (1 1 n ) = F 1 (1 1 ne ) F 1 (1 1 n ) where F 1 is the inverse funtion. It is known that the df of a χ 2 2p random variable is equal to F (x) = 1 e x e p (x), where e p (x) = p 1 k=0 xk k!. Choosing = log n + log(log( np 1 (p 1)! )) and = 1 we have: lim F n ( + x) = exp( e x ) (20) n

10 10 We use (20) to evaluate the logarithmi moment of χ 2 p,n whih is key to our analysis. In the above formulation we hoose F to be the df of a hi-square random variable with p degrees of freedom. Jensen s inequality provides an upper bound on the logarithmi moment and furthermore the following theorem states that this bound is asymptotially tight. Theorem 2: Let {X n } n be positive random variables with finite mean and variane, X (n), W, { } and { > 0} are defined as in Theorem 1 and furthermore, an, then as n : Proof: See Appendix. log(e[x (n) ) E[log X (n) 0 So to alulate the logarithmi moment it is suffiient to only evaluate the mean of the above random variable. It is known that when the limiting distribution is of the first kind (Gumbel distribution) then Theorem 1 an also be used to evaluate the moments of X (n) (in fat for this ase, onvergene in distribution implies onvergene in moments [22). In partiular we have [ X(n) E E[W = γ (21) E [ (X(n) ) a 2 n E[W 2 = π2 6 Hene, the asymptoti growth of the logarithmi moment of the extreme order statistis of hi-square random variables is given by (22) E[log(X (n) ) = log(e[x (n) ) = log (log n + log(log( np 1 (p 1)! )) + γ = log(log n) (23) ) Now we an evaluate the behavior of G in (17): Hene G = = N E[log( χ 2 2(N i+1),m i+1 ) N log N (M i+1)n i N log(m i + 1) + log(log( log (N i)! )) + γ (24) N G = N log(log M)

11 Capaity gain (N=2, SNR=30 db) 2 Spetral effiieny (Nats/Se/Hz) Asymptoti Approximation Monte Carlo simulation Number of transmit antennas (M) Fig. 3. Capaity gain of antenna seletion (N=2 and SNR=30 db) Thus the apaity gain for transmit antenna seletion behaves like O (log(log M)). Also, for large number of transmit antennas Eq. 24 an be used as an approximate formula for ergodi apaity of transmit antenna seletion at high SNR, in fat C N log ρ + G (25) Figure 3 ompares our result with omputer simulations. We run the simulation for SNR=30 db and N=2. For eah point on the plot, the apaity gain is alulated by averaging over 5000 different hannel realizations and ompared to the results obtained from equation (24). Simulations math our analysis very well, thus the asymptoti formula proves to be a useful tool for the evaluating of the apaity of transmit antenna seletion. V. TRANSMIT ANTENNA SELECTION: LOW SNR CASE For low SNR ase, we use the onept of hannel gain, introdued by Verdu [1, whih is essentially the slope of the linear term in the Taylor expansion of the ergodi apaity, namely, Γ = C(ρ) ρ (26) ρ=0 sine C = Γ ρ+o(ρ 2 ), Γ an be onsidered as an information theoreti metri for evaluating the spetral effiieny at low SNR [1.

12 12 Uninformed transmitter: In this ase the hannel gain [1 is: [ H 2 Γ = E F = N (27) M we notie that in this ase the hannel gain does not depend on M, so inreasing the number of transmit antenna will not affet the apaity. Informed transmitter: When CSI is fully provided at the transmitter, at low SNR, the beamformer only uses the eigen mode of the hannel assoiated with the largest eigen value of H H H hene the hannel gain is [1: Γ wf = E[λ max (H H H) (28) It was first shown in [23 that λ max = ( M + N) 2 when M or N are large. Thus for the ase M N, we have Γ wf = M. Antenna seletion: Suppose we are seleting L transmit antennas with equal power splitting among them. In low SNR senario, the hannel gain is: [ Γ = H 2 F E L = E[ L h i 2 2 L where H is the seleted hannel, and h 1,..., h L are the L olumns of H. Thus antenna seletion in low SNR ase leads to seleting L antennas with highest norm. This is also onsistent with the suessive antenna seletion algorithm presented in Figure 1 for ρ 0. Moreover, the hannel gain is maximized when L = 1, beause E[ L h i 2 2 L max i { h i 2 2 }. This suggests that the optimal transmit antenna seletion strategy in low SNR ase is to selet only one transmit antenna whose hannel vetor is of the highest norm. In other words H = h j where h j = max{ h 1,..., h M }. Now in order to evaluate the hannel gain for low SNR transmit antenna seletion we need to evaluate E[ H 2 F. The random variable H 2 F is distributed aording to X 2N,M defined in Setion III-A. For M N, using Theorem 1 we have: Γ opt = log M + log(log( M N 1 (N 1)! )) + γ = log M (29) VI. RECEIVE ANTENNA SELECTION Up to this point, the emphasis of the paper has been on the transmitter side. However, it is not diffiult to see that due to the reiproity of eletromagneti propagation, the problem is highly symmetri, therefore we an use the framework developed thus far to also address reeive antenna seletion.

13 13 In partiular, onsider the following setup: A MIMO system with M transmit and N reeive antennas, suh that N M. We wish to hoose L out of N reeive antennas in a way to maximize the retained apaity. The algorithm depited in Figure 1 will perform the antenna seletion, with the notable differene that we now must selet rows and not olumns of H. As before, we all the seleted hannel H. Assuming reeive antenna seletion with L = M and no CSI at transmitter, the apaity of the system is: Similarly to the previous ase, we an write: C = log det(i L + ρ M H H H ) log det(i + ρ M H H M H ) log (1 + ρ M χ2 2M,N i+1) M log ρ M log M + = M log ρ + Ĝ M log χ 2 2M,N i+1 where χ 2 2M,N i+1 is as earlier defined, the maximum of N i + 1 hi-square random variables. Reall that in transmit seletion the SNR sales by the fator ρ/l in Equation (2), i.e., the fewer the seleted antennas, the more power an be sent through eah antenna. The result was that the apaity atually inreases through transmit antenna seletion, 4 an inrease that was haraterized by G. In reeive seletion, seleting fewer antennas will result in smaller reeive power, but antennas that are seleted enjoy better hannel distributions than the original MIMO hannel. However, the loss of power annot be made up by the improvement in the hannel distributions. Therefore the apaity of the reeive antenna seletion is less than the apaity of the full-sale system. Unlike transmit seletion, no additional apaity is obtained by seleting down to the best antennas, a result that is not surprising beause information is being lost by reeive seletion. The above results are demonstrated on a 2 8 system in Figure 4. In the low-snr regime, we one again use the onept of hannel gain, whih for the reeive antenna seletion leads to: [ Γ = H [ L 2 F E = E h i 2 2 M M 4 Assuming the multiplexing gain of the system is unaffeted by seletion, whih we ensured via our transmit-seletion assumption of N L M

14 Spetral Effiieny (bits/se/hz) SNR (db) No Seletion Rx Seletion Fig. 4. Reeive antenna seletion in a 2 8 system It is evident that, unlike the transmit-seletion ase, there is no penalty for seleting more antennas, in fat the more antennas seleted, the higher the apaity. Calulating this value using Theorem 1 we have Γ = L M log N (30) VII. CONCLUSION In this paper, we investigate the behavior of the apaity of antenna seletion in the asymptote of large number of transmit antennas. For high SNR ase, we introdue the onept of apaity gain, an information theoreti metri for shemes that use hannel state information at the transmitter. It is shown that this quantity desribes the advantage gained by having hannel state information at the transmitter. We present new results in order statistis that are useful for asymptoti analysis of antenna seletion problems. By exploring the behavior of the apaity gain, we show that the optimal number of seleted antennas for large M is exatly N. Simulations show that the analysis is aurate and an be used for approximation of the apaity of antenna seletion. For low SNR ase, we first show that the optimal seletion strategy is to selet only one transmit antenna with the highest hannel norm. Also, we evaluate the hannel gain and show its logarithmi behavior in the asymptote of large number of antennas. VIII. APPENDIX Lemma 1: If an ( ) X(n) d, then log 0.

15 15 Proof: For every ɛ > 0 and δ > 0 [ [ X (n) P r 1 > ɛ X (n) = P r > ɛ [ ( ) X(n) a 2 E n ɛ 2 ( an ) 2 < E[W 2 + δ ɛ 2 ( an ) 2 0 as n. Thus X(n) onlude that log i.p. 1, hene X(n) ( X(n) ) d 0. Lemma 2: Let µ n = E[X (n), if Proof: From Eq. (21) we have µn an b ( ) n µ n 1 0, hene log an µ n 0. d 1. Now using the ontinous mapping theorem [24 we ( ), then log µn 0. 0, also we have bn 0. By multiplying two sides we get Definition 2: The sequene of random varibales {X n } is alled uniformly integrable if [24: lim lim sup x df Xn (x) < (31) n X n > Lemma 3: If the random variables {X n } have finite mean, then the uniform integrability is equivalent to the following ondition: lim lim sup n X n > Proof: Using integration by part we have x df Xn (x) = x(1 F Xn (x)) + X n > Pr[ X n > xdx < (32) Sine E[X n <, we have lim (1 F Xn ()) = 0 and this proves the lemma. Pr[ X n > xdx (33) Theorem 3: If the sequane of random variables {X n } is uniformly integrable, then X n E[X n E[X. Proof: See [24. d X implies ( ) Proof of Theorem 2: Let Y n = log Xn d, then by Lemma 1 we have Y n 0, we show that Y n is uniformly integrable, and to do so we use the alternative form of uniform integrability provided by Lemma 2: Pr[ Y n > ydy = Pr[Y n > ydy + Pr[Y n < ydy = I 1 + I 2 (34)

16 16 We evaluate eah integral, Let η n = bn I 1 = = = = α Pr[Y n > ydy Pr[X n > e y dy [ Xn Pr > a n (e y 1) dy [ Xn Pr > a n dt t, t := e y 1, α = e 1 (35) t + 1 [ ( ) 2 Xn π2 6. Thus using therefore η n as n. From Eq. (22) we have E Chebyshev s inequality, for every δ > 0 we have: Also in a similar way for all δ > 0 we have, I 2 = = = = ( bn ( bn ( bn [ ( ) 2 I 1 1 E Xn ηn 2 α t 2 dt (t + 1) 1 π 2 /6 + δ ηn 2 α t 2 (t + 1) dt 1 η 2 n(α + 1) α π 2 /6 + δ t 2 dt = π2 /6 + δ ηnα(α 2 0 (36) + 1) Pr[Y n < ydy Pr[X n < e y dy [ an X n Pr ) 2 ) 2 ) 2 ( π2 6 + δ) > a n (1 e y ) dy E[( an X n ) 2 (1 e y ) 2 dy π δ (1 e y ) 2 dy ( ) e 1 e + log(1 e ) 0 (37) from Eq. (36) and (37) we onlude that I 1 + I 2 0 thus, Y n is uniformly integrable hene Y n onverges in mean, namely, E[log X (n) log 0. On the other hand, by Lemma 2 we have log(e[x (n) ) log 0 thus we have E[log X (n) log(e[x (n) ) 0.

17 17 REFERENCES [1 S. Verdu, Spetral effiieny in wideband regime, IEEE Trans. on Information Theory, vol. 48, no. 6, pp , June [2 S. Sanayei and A. Nosratinia, Antenna seletion in MIMO systems, IEEE Communiations Magazine, vol. 42, no. 10, pp , Ot [3 M. Z. Win and J. H. Winters, Analysis of hybrid seletion/maximal ratio ombining in Rayleigh fading, IEEE Trans. on Communiations, vol. 47, pp , De [4 R. Heath and A. Paulraj, Antenna seletion for spatial multiplexing systems based on minimum error rate, in Pro. International Conferene on Communiations, Helsinki, Finland, June 2003, pp [5 D. Gore, R. U. Nabar, and A. Paulraj, Seleting an optimal set of transmit antennas for a low rank matrix hannel, in Pro. IEEE ICASSP, Istanbul, Turkey, May 2000, pp [6 R. S. Blum and J. H. Winters, On optimum mimo with antenna seletion, IEEE Communiations Letters, vol. 6, pp , Aug [7 D. Gore, R. Heath, and A. Paulraj, Transmit seletion in spatial multiplexing systems, IEEE Communiations Letters, vol. 6, no. 1, pp , Nov [8 S. Sanayei and A. Nosratinia, Asymptoti apaity gain of transmit antenna seletion, in Pro. WNCG Symposium, Austin, TX, Ot [9 S. Sanayei and A. Nosratinia, Asymptoti apaity analysis of transmit antenna seletion, in Pro. of IEEE International Symposium on Information Theory, Chiago, IL, June 2004, p [10 A. Gorokhov, Antenna seletion algorithms for mea transmission systems, in Pro. IEEE ICASSP, Orlando, FL, May 2002, pp [11 A. Gorokhov, D. A. Gore, and A. J. Paulraj, Reeive antenna seletion for MIMO spatial multiplexing: Theory and algorithms, IEEE Trans. on Signal Proessing, pp , Nov [12 M. Gharavi-Alkhansari and A. Greshman, Fast antenna seletion in MIMO systems, IEEE Trans. on Signal Proessing, vol. 52, no. 2, pp , Feb [13 A. Gorokhov, D. Gore, and A. Paulraj, Reeive antenna seletion for MIMO flat fading hannels: theory and algorithms, IEEE Trans. on Information Theory, vol. 49, no. 10, pp , Ot [14 M. Win, A. Molish, and Winters, Capaity of MIMO systems with antenna seletion, in Pro. International Conferene on Communiations, 2001, vol. 2, pp [15 A. Lozano, A. Tulino, and S. Verdu, High-SNR power offset in multi-antenna ommuniation, in Pro. of IEEE International Symposium on Information Theory, Chiago, IL, June 2004, p [16 D. Bliss, K. Forsythe, A. Hero, and A. Yegulalp, Environmental issues for MIMO apaity, IEEE Trans. on Signal Proessing, vol. 50, no. 9, pp , September [17 G. Kéri, The Sherman-Morisson formula for the determinant and its appliation for optimizing the quadrati funtions on onditinos sets given by extreme generators, in Optimization Theory: Reent Developments from Mátraháza, F. Giannessi, P. Pardalos, and T. Rapsàk, Eds. Kluwer, [18 B. C. Arnold, N. Balakrishnan, and H. N. Nagaraja, A first ourse in order statistis, John Wiley and Sons, [19 I. E. Telatar, Capaity of multi-antenna Gaussian hannels, European Trans. on Teleommuniation, vol. 10, pp , Nov

18 18 [20 G. J. Foshini and M. J. Gans, On limits of wireless ommuniation in fading environment when using multiple antennas, Wireless Personal Communiation, vol. 6, pp , Marh [21 O. Oyman, R. U. Nabar, H. Bolskei, and A. J. Paulraj, Charaterizing the statistial properties of mutual information in MIMO hannels: Insights into diversity-multiplexing tradeoff, IEEE Trans. on Signal Proessing, vol. 51, no. 11, pp , Nov [22 J. Galambos, Asymptoti Theory of Order Statistis, Krieger Pub. Co., [23 S. Geman, A limit theorem for the norm of the random matries, Annals of probability, vol. 8, pp , [24 P. Billingsley, Probability and Measure, Wiley, 1995.

Capacity-achieving Input Covariance for Correlated Multi-Antenna Channels

Capacity-achieving Input Covariance for Correlated Multi-Antenna Channels Capaity-ahieving Input Covariane for Correlated Multi-Antenna Channels Antonia M. Tulino Universita Degli Studi di Napoli Federio II 85 Napoli, Italy atulino@ee.prineton.edu Angel Lozano Bell Labs (Luent

More information

Case I: 2 users In case of 2 users, the probability of error for user 1 was earlier derived to be 2 A1

Case I: 2 users In case of 2 users, the probability of error for user 1 was earlier derived to be 2 A1 MUTLIUSER DETECTION (Letures 9 and 0) 6:33:546 Wireless Communiations Tehnologies Instrutor: Dr. Narayan Mandayam Summary By Shweta Shrivastava (shwetash@winlab.rutgers.edu) bstrat This artile ontinues

More information

IN opportunistic beamforming [1] the base-station acquires

IN opportunistic beamforming [1] the base-station acquires IEEE TRANSACTIONS ON WIRELESS COMMUNICATIONS, VOL. 6, NO. 8, AUGUST 27 2765 Opportunisti Beamforming with Limited Feedbak Shahab Sanayei, Member, IEEE, and Aria Nosratinia, Senior Member, IEEE Abstrat

More information

Hankel Optimal Model Order Reduction 1

Hankel Optimal Model Order Reduction 1 Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both

More information

Lecture 7: Sampling/Projections for Least-squares Approximation, Cont. 7 Sampling/Projections for Least-squares Approximation, Cont.

Lecture 7: Sampling/Projections for Least-squares Approximation, Cont. 7 Sampling/Projections for Least-squares Approximation, Cont. Stat60/CS94: Randomized Algorithms for Matries and Data Leture 7-09/5/013 Leture 7: Sampling/Projetions for Least-squares Approximation, Cont. Leturer: Mihael Mahoney Sribe: Mihael Mahoney Warning: these

More information

SURFACE WAVES OF NON-RAYLEIGH TYPE

SURFACE WAVES OF NON-RAYLEIGH TYPE SURFACE WAVES OF NON-RAYLEIGH TYPE by SERGEY V. KUZNETSOV Institute for Problems in Mehanis Prosp. Vernadskogo, 0, Mosow, 75 Russia e-mail: sv@kuznetsov.msk.ru Abstrat. Existene of surfae waves of non-rayleigh

More information

Chapter Review of of Random Processes

Chapter Review of of Random Processes Chapter.. Review of of Random Proesses Random Variables and Error Funtions Conepts of Random Proesses 3 Wide-sense Stationary Proesses and Transmission over LTI 4 White Gaussian Noise Proesses @G.Gong

More information

Advances in Radio Science

Advances in Radio Science Advanes in adio Siene 2003) 1: 99 104 Copernius GmbH 2003 Advanes in adio Siene A hybrid method ombining the FDTD and a time domain boundary-integral equation marhing-on-in-time algorithm A Beker and V

More information

The Capacity Loss of Dense Constellations

The Capacity Loss of Dense Constellations The Capaity Loss of Dense Constellations Tobias Koh University of Cambridge tobi.koh@eng.am.a.uk Alfonso Martinez Universitat Pompeu Fabra alfonso.martinez@ieee.org Albert Guillén i Fàbregas ICREA & Universitat

More information

Research Collection. Mismatched decoding for the relay channel. Conference Paper. ETH Library. Author(s): Hucher, Charlotte; Sadeghi, Parastoo

Research Collection. Mismatched decoding for the relay channel. Conference Paper. ETH Library. Author(s): Hucher, Charlotte; Sadeghi, Parastoo Researh Colletion Conferene Paper Mismathed deoding for the relay hannel Author(s): Huher, Charlotte; Sadeghi, Parastoo Publiation Date: 2010 Permanent Link: https://doi.org/10.3929/ethz-a-005997152 Rights

More information

Enhanced Max-Min SINR for Uplink Cell-Free Massive MIMO Systems

Enhanced Max-Min SINR for Uplink Cell-Free Massive MIMO Systems Enhaned Max-Min SINR for Uplin Cell-Free Massive MIMO Systems Manijeh Bashar, Kanapathippillai Cumanan, Alister G. Burr,Mérouane Debbah, and Hien Quo Ngo Department of Eletroni Engineering, University

More information

Control Theory association of mathematics and engineering

Control Theory association of mathematics and engineering Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology

More information

Advanced Computational Fluid Dynamics AA215A Lecture 4

Advanced Computational Fluid Dynamics AA215A Lecture 4 Advaned Computational Fluid Dynamis AA5A Leture 4 Antony Jameson Winter Quarter,, Stanford, CA Abstrat Leture 4 overs analysis of the equations of gas dynamis Contents Analysis of the equations of gas

More information

23.1 Tuning controllers, in the large view Quoting from Section 16.7:

23.1 Tuning controllers, in the large view Quoting from Section 16.7: Lesson 23. Tuning a real ontroller - modeling, proess identifiation, fine tuning 23.0 Context We have learned to view proesses as dynami systems, taking are to identify their input, intermediate, and output

More information

Frequency hopping does not increase anti-jamming resilience of wireless channels

Frequency hopping does not increase anti-jamming resilience of wireless channels Frequeny hopping does not inrease anti-jamming resiliene of wireless hannels Moritz Wiese and Panos Papadimitratos Networed Systems Seurity Group KTH Royal Institute of Tehnology, Stoholm, Sweden {moritzw,

More information

The Effectiveness of the Linear Hull Effect

The Effectiveness of the Linear Hull Effect The Effetiveness of the Linear Hull Effet S. Murphy Tehnial Report RHUL MA 009 9 6 Otober 009 Department of Mathematis Royal Holloway, University of London Egham, Surrey TW0 0EX, England http://www.rhul.a.uk/mathematis/tehreports

More information

Tests of fit for symmetric variance gamma distributions

Tests of fit for symmetric variance gamma distributions Tests of fit for symmetri variane gamma distributions Fragiadakis Kostas UADPhilEon, National and Kapodistrian University of Athens, 4 Euripidou Street, 05 59 Athens, Greee. Keywords: Variane Gamma Distribution,

More information

Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite.

Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite. Leture Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the funtion V ( x ) to be positive definite. ost often, our interest will be to show that x( t) as t. For that we will need

More information

Tight Lower Bounds on the Ergodic Capacity of Rayleigh Fading MIMO Channels

Tight Lower Bounds on the Ergodic Capacity of Rayleigh Fading MIMO Channels Tight Lower Bounds on the Ergodic Capacity of Rayleigh Fading MIMO Channels Özgür Oyman ), Rohit U. Nabar ), Helmut Bölcskei 2), and Arogyaswami J. Paulraj ) ) Information Systems Laboratory, Stanford

More information

Robust Recovery of Signals From a Structured Union of Subspaces

Robust Recovery of Signals From a Structured Union of Subspaces Robust Reovery of Signals From a Strutured Union of Subspaes 1 Yonina C. Eldar, Senior Member, IEEE and Moshe Mishali, Student Member, IEEE arxiv:87.4581v2 [nlin.cg] 3 Mar 29 Abstrat Traditional sampling

More information

Journal of Inequalities in Pure and Applied Mathematics

Journal of Inequalities in Pure and Applied Mathematics Journal of Inequalities in Pure and Applied Mathematis A NEW ARRANGEMENT INEQUALITY MOHAMMAD JAVAHERI University of Oregon Department of Mathematis Fenton Hall, Eugene, OR 97403. EMail: javaheri@uoregon.edu

More information

Sensitivity of Spectrum Sensing Techniques to RF impairments

Sensitivity of Spectrum Sensing Techniques to RF impairments Sensitivity of Spetrum Sensing Tehniques to RF impairments Jonathan Verlant-Chenet Julien Renard Jean-Mihel Driot Philippe De Donker François Horlin Université Libre de Bruelles - OPERA Dpt., Avenue F.D.

More information

Lightpath routing for maximum reliability in optical mesh networks

Lightpath routing for maximum reliability in optical mesh networks Vol. 7, No. 5 / May 2008 / JOURNAL OF OPTICAL NETWORKING 449 Lightpath routing for maximum reliability in optial mesh networks Shengli Yuan, 1, * Saket Varma, 2 and Jason P. Jue 2 1 Department of Computer

More information

Complexity of Regularization RBF Networks

Complexity of Regularization RBF Networks Complexity of Regularization RBF Networks Mark A Kon Department of Mathematis and Statistis Boston University Boston, MA 02215 mkon@buedu Leszek Plaskota Institute of Applied Mathematis University of Warsaw

More information

ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS

ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS MARIO LEFEBVRE and JEAN-LUC GUILBAULT A ontinuous-time and ontinuous-state stohasti proess, denoted by {Xt), t }, is defined from a proess known as

More information

(q) -convergence. Comenius University, Bratislava, Slovakia

(q) -convergence.   Comenius University, Bratislava, Slovakia Annales Mathematiae et Informatiae 38 (2011) pp. 27 36 http://ami.ektf.hu On I (q) -onvergene J. Gogola a, M. Mačaj b, T. Visnyai b a University of Eonomis, Bratislava, Slovakia e-mail: gogola@euba.sk

More information

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013 Ultrafast Pulses and GVD John O Hara Created: De. 6, 3 Introdution This doument overs the basi onepts of group veloity dispersion (GVD) and ultrafast pulse propagation in an optial fiber. Neessarily, it

More information

CMSC 451: Lecture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017

CMSC 451: Lecture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017 CMSC 451: Leture 9 Greedy Approximation: Set Cover Thursday, Sep 28, 2017 Reading: Chapt 11 of KT and Set 54 of DPV Set Cover: An important lass of optimization problems involves overing a ertain domain,

More information

Diversity Analysis of Bit-Interleaved Coded Multiple Beamforming with Orthogonal Frequency Division Multiplexing

Diversity Analysis of Bit-Interleaved Coded Multiple Beamforming with Orthogonal Frequency Division Multiplexing IEEE ICC 03 - Wireless Communiations Symposium Diversity Analysis of Bit-Interleaved Coded Multiple Beamforming with Orthogonal Frequeny Division Multiplexing Boyu Li and Ender Ayanoglu Center for Pervasive

More information

SINCE Zadeh s compositional rule of fuzzy inference

SINCE Zadeh s compositional rule of fuzzy inference IEEE TRANSACTIONS ON FUZZY SYSTEMS, VOL. 14, NO. 6, DECEMBER 2006 709 Error Estimation of Perturbations Under CRI Guosheng Cheng Yuxi Fu Abstrat The analysis of stability robustness of fuzzy reasoning

More information

Maximum Entropy and Exponential Families

Maximum Entropy and Exponential Families Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It

More information

Phase Diffuser at the Transmitter for Lasercom Link: Effect of Partially Coherent Beam on the Bit-Error Rate.

Phase Diffuser at the Transmitter for Lasercom Link: Effect of Partially Coherent Beam on the Bit-Error Rate. Phase Diffuser at the Transmitter for Laserom Link: Effet of Partially Coherent Beam on the Bit-Error Rate. O. Korotkova* a, L. C. Andrews** a, R. L. Phillips*** b a Dept. of Mathematis, Univ. of Central

More information

Spatial Degrees of Freedom of Large Distributed MIMO Systems and Wireless Ad hoc Networks

Spatial Degrees of Freedom of Large Distributed MIMO Systems and Wireless Ad hoc Networks Spatial Degrees of Freedom of Large Distributed MIMO Systems and Wireless Ad ho Networks Ayfer Özgür Stanford University aozgur@stanford.edu Olivier Lévêque EPFL, Switzerland olivier.leveque@epfl.h David

More information

Assessing the Performance of a BCI: A Task-Oriented Approach

Assessing the Performance of a BCI: A Task-Oriented Approach Assessing the Performane of a BCI: A Task-Oriented Approah B. Dal Seno, L. Mainardi 2, M. Matteui Department of Eletronis and Information, IIT-Unit, Politenio di Milano, Italy 2 Department of Bioengineering,

More information

A Spatiotemporal Approach to Passive Sound Source Localization

A Spatiotemporal Approach to Passive Sound Source Localization A Spatiotemporal Approah Passive Sound Soure Loalization Pasi Pertilä, Mikko Parviainen, Teemu Korhonen and Ari Visa Institute of Signal Proessing Tampere University of Tehnology, P.O.Box 553, FIN-330,

More information

Space-time duality in multiple antenna channels

Space-time duality in multiple antenna channels Spae-time duality in multiple antenna hannels Massimo Franeshetti, Kaushik Chakraborty 1 Abstrat The onept of information transmission in a multiple antenna hannel with sattering objets is studied from

More information

Single-User MIMO systems: Introduction, capacity results, and MIMO beamforming

Single-User MIMO systems: Introduction, capacity results, and MIMO beamforming Single-User MIMO systems: Introduction, capacity results, and MIMO beamforming Master Universitario en Ingeniería de Telecomunicación I. Santamaría Universidad de Cantabria Contents Introduction Multiplexing,

More information

Directional Coupler. 4-port Network

Directional Coupler. 4-port Network Diretional Coupler 4-port Network 3 4 A diretional oupler is a 4-port network exhibiting: All ports mathed on the referene load (i.e. S =S =S 33 =S 44 =0) Two pair of ports unoupled (i.e. the orresponding

More information

A Queueing Model for Call Blending in Call Centers

A Queueing Model for Call Blending in Call Centers A Queueing Model for Call Blending in Call Centers Sandjai Bhulai and Ger Koole Vrije Universiteit Amsterdam Faulty of Sienes De Boelelaan 1081a 1081 HV Amsterdam The Netherlands E-mail: {sbhulai, koole}@s.vu.nl

More information

On Molecular Timing Channels with α-stable Noise

On Molecular Timing Channels with α-stable Noise On Moleular Timing Channels with α-stable Noise Yonathan Murin, Nariman Farsad, Mainak Chowdhury, and Andrea Goldsmith Department of Eletrial Engineering, Stanford University, USA Abstrat This work studies

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

On the Bit Error Probability of Noisy Channel Networks With Intermediate Node Encoding I. INTRODUCTION

On the Bit Error Probability of Noisy Channel Networks With Intermediate Node Encoding I. INTRODUCTION 5188 IEEE TRANSACTIONS ON INFORMATION THEORY, VOL. 54, NO. 11, NOVEMBER 2008 [8] A. P. Dempster, N. M. Laird, and D. B. Rubin, Maximum likelihood estimation from inomplete data via the EM algorithm, J.

More information

A Characterization of Wavelet Convergence in Sobolev Spaces

A Characterization of Wavelet Convergence in Sobolev Spaces A Charaterization of Wavelet Convergene in Sobolev Spaes Mark A. Kon 1 oston University Louise Arakelian Raphael Howard University Dediated to Prof. Robert Carroll on the oasion of his 70th birthday. Abstrat

More information

LECTURE NOTES FOR , FALL 2004

LECTURE NOTES FOR , FALL 2004 LECTURE NOTES FOR 18.155, FALL 2004 83 12. Cone support and wavefront set In disussing the singular support of a tempered distibution above, notie that singsupp(u) = only implies that u C (R n ), not as

More information

Developing Excel Macros for Solving Heat Diffusion Problems

Developing Excel Macros for Solving Heat Diffusion Problems Session 50 Developing Exel Maros for Solving Heat Diffusion Problems N. N. Sarker and M. A. Ketkar Department of Engineering Tehnology Prairie View A&M University Prairie View, TX 77446 Abstrat This paper

More information

Geometry of Transformations of Random Variables

Geometry of Transformations of Random Variables Geometry of Transformations of Random Variables Univariate distributions We are interested in the problem of finding the distribution of Y = h(x) when the transformation h is one-to-one so that there is

More information

Product Policy in Markets with Word-of-Mouth Communication. Technical Appendix

Product Policy in Markets with Word-of-Mouth Communication. Technical Appendix rodut oliy in Markets with Word-of-Mouth Communiation Tehnial Appendix August 05 Miro-Model for Inreasing Awareness In the paper, we make the assumption that awareness is inreasing in ustomer type. I.e.,

More information

Exploiting Partial Channel Knowledge at the Transmitter in MISO and MIMO Wireless

Exploiting Partial Channel Knowledge at the Transmitter in MISO and MIMO Wireless Exploiting Partial Channel Knowledge at the Transmitter in MISO and MIMO Wireless SPAWC 2003 Rome, Italy June 18, 2003 E. Yoon, M. Vu and Arogyaswami Paulraj Stanford University Page 1 Outline Introduction

More information

Stability of alternate dual frames

Stability of alternate dual frames Stability of alternate dual frames Ali Akbar Arefijamaal Abstrat. The stability of frames under perturbations, whih is important in appliations, is studied by many authors. It is worthwhile to onsider

More information

EECS 120 Signals & Systems University of California, Berkeley: Fall 2005 Gastpar November 16, Solutions to Exam 2

EECS 120 Signals & Systems University of California, Berkeley: Fall 2005 Gastpar November 16, Solutions to Exam 2 EECS 0 Signals & Systems University of California, Berkeley: Fall 005 Gastpar November 6, 005 Solutions to Exam Last name First name SID You have hour and 45 minutes to omplete this exam. he exam is losed-book

More information

Nonreversibility of Multiple Unicast Networks

Nonreversibility of Multiple Unicast Networks Nonreversibility of Multiple Uniast Networks Randall Dougherty and Kenneth Zeger September 27, 2005 Abstrat We prove that for any finite direted ayli network, there exists a orresponding multiple uniast

More information

Sensor management for PRF selection in the track-before-detect context

Sensor management for PRF selection in the track-before-detect context Sensor management for PRF seletion in the tra-before-detet ontext Fotios Katsilieris, Yvo Boers, and Hans Driessen Thales Nederland B.V. Haasbergerstraat 49, 7554 PA Hengelo, the Netherlands Email: {Fotios.Katsilieris,

More information

arxiv:math/ v1 [math.ca] 27 Nov 2003

arxiv:math/ v1 [math.ca] 27 Nov 2003 arxiv:math/011510v1 [math.ca] 27 Nov 200 Counting Integral Lamé Equations by Means of Dessins d Enfants Sander Dahmen November 27, 200 Abstrat We obtain an expliit formula for the number of Lamé equations

More information

A variant of Coppersmith s Algorithm with Improved Complexity and Efficient Exhaustive Search

A variant of Coppersmith s Algorithm with Improved Complexity and Efficient Exhaustive Search A variant of Coppersmith s Algorithm with Improved Complexity and Effiient Exhaustive Searh Jean-Sébastien Coron 1, Jean-Charles Faugère 2, Guénaël Renault 2, and Rina Zeitoun 2,3 1 University of Luxembourg

More information

Wave Propagation through Random Media

Wave Propagation through Random Media Chapter 3. Wave Propagation through Random Media 3. Charateristis of Wave Behavior Sound propagation through random media is the entral part of this investigation. This hapter presents a frame of referene

More information

Sensor Network Localisation with Wrapped Phase Measurements

Sensor Network Localisation with Wrapped Phase Measurements Sensor Network Loalisation with Wrapped Phase Measurements Wenhao Li #1, Xuezhi Wang 2, Bill Moran 2 # Shool of Automation, Northwestern Polytehnial University, Xian, P.R.China. 1. wenhao23@mail.nwpu.edu.n

More information

Chapter 8 Hypothesis Testing

Chapter 8 Hypothesis Testing Leture 5 for BST 63: Statistial Theory II Kui Zhang, Spring Chapter 8 Hypothesis Testing Setion 8 Introdution Definition 8 A hypothesis is a statement about a population parameter Definition 8 The two

More information

Connectivity and Blockage Effects in Millimeter-Wave Air-To-Everything Networks

Connectivity and Blockage Effects in Millimeter-Wave Air-To-Everything Networks 1 Connetivity and Blokage Effets in Millimeter-Wave Air-To-Everything Networks Kaifeng Han, Kaibin Huang and Robert W. Heath Jr. arxiv:1808.00144v1 [s.it] 1 Aug 2018 Abstrat Millimeter-wave (mmwave) offers

More information

The Hanging Chain. John McCuan. January 19, 2006

The Hanging Chain. John McCuan. January 19, 2006 The Hanging Chain John MCuan January 19, 2006 1 Introdution We onsider a hain of length L attahed to two points (a, u a and (b, u b in the plane. It is assumed that the hain hangs in the plane under a

More information

Title. Author(s)Tsai, Shang-Ho. Issue Date Doc URL. Type. Note. File Information. Equal Gain Beamforming in Rayleigh Fading Channels

Title. Author(s)Tsai, Shang-Ho. Issue Date Doc URL. Type. Note. File Information. Equal Gain Beamforming in Rayleigh Fading Channels Title Equal Gain Beamforming in Rayleigh Fading Channels Author(s)Tsai, Shang-Ho Proceedings : APSIPA ASC 29 : Asia-Pacific Signal Citationand Conference: 688-691 Issue Date 29-1-4 Doc URL http://hdl.handle.net/2115/39789

More information

Taste for variety and optimum product diversity in an open economy

Taste for variety and optimum product diversity in an open economy Taste for variety and optimum produt diversity in an open eonomy Javier Coto-Martínez City University Paul Levine University of Surrey Otober 0, 005 María D.C. Garía-Alonso University of Kent Abstrat We

More information

Normative and descriptive approaches to multiattribute decision making

Normative and descriptive approaches to multiattribute decision making De. 009, Volume 8, No. (Serial No.78) China-USA Business Review, ISSN 57-54, USA Normative and desriptive approahes to multiattribute deision making Milan Terek (Department of Statistis, University of

More information

Multiple Antennas in Wireless Communications

Multiple Antennas in Wireless Communications Multiple Antennas in Wireless Communications Luca Sanguinetti Department of Information Engineering Pisa University luca.sanguinetti@iet.unipi.it April, 2009 Luca Sanguinetti (IET) MIMO April, 2009 1 /

More information

SPLINE ESTIMATION OF SINGLE-INDEX MODELS

SPLINE ESTIMATION OF SINGLE-INDEX MODELS SPLINE ESIMAION OF SINGLE-INDEX MODELS Li Wang and Lijian Yang University of Georgia and Mihigan State University Supplementary Material his note ontains proofs for the main results he following two propositions

More information

Word of Mass: The Relationship between Mass Media and Word-of-Mouth

Word of Mass: The Relationship between Mass Media and Word-of-Mouth Word of Mass: The Relationship between Mass Media and Word-of-Mouth Roman Chuhay Preliminary version Marh 6, 015 Abstrat This paper studies the optimal priing and advertising strategies of a firm in the

More information

Computer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1

Computer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1 Computer Siene 786S - Statistial Methods in Natural Language Proessing and Data Analysis Page 1 Hypothesis Testing A statistial hypothesis is a statement about the nature of the distribution of a random

More information

The law of the iterated logarithm for c k f(n k x)

The law of the iterated logarithm for c k f(n k x) The law of the iterated logarithm for k fn k x) Christoph Aistleitner Abstrat By a lassial heuristis, systems of the form osπn k x) k 1 and fn k x)) k 1, where n k ) k 1 is a rapidly growing sequene of

More information

Methods of evaluating tests

Methods of evaluating tests Methods of evaluating tests Let X,, 1 Xn be i.i.d. Bernoulli( p ). Then 5 j= 1 j ( 5, ) T = X Binomial p. We test 1 H : p vs. 1 1 H : p>. We saw that a LRT is 1 if t k* φ ( x ) =. otherwise (t is the observed

More information

LOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION

LOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION LOGISIC REGRESSIO I DEPRESSIO CLASSIFICAIO J. Kual,. V. ran, M. Bareš KSE, FJFI, CVU v Praze PCP, CS, 3LF UK v Praze Abstrat Well nown logisti regression and the other binary response models an be used

More information

Estimating the probability law of the codelength as a function of the approximation error in image compression

Estimating the probability law of the codelength as a function of the approximation error in image compression Estimating the probability law of the odelength as a funtion of the approximation error in image ompression François Malgouyres Marh 7, 2007 Abstrat After some reolletions on ompression of images using

More information

Time Domain Method of Moments

Time Domain Method of Moments Time Domain Method of Moments Massahusetts Institute of Tehnology 6.635 leture notes 1 Introdution The Method of Moments (MoM) introdued in the previous leture is widely used for solving integral equations

More information

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b Consider the pure initial value problem for a homogeneous system of onservation laws with no soure terms in one spae dimension: Where as disussed previously we interpret solutions to this partial differential

More information

Broadcast Channels with Cooperating Decoders

Broadcast Channels with Cooperating Decoders To appear in the IEEE Transations on Information Theory, Deember 2006. 1 Broadast Channels with Cooperating Deoders Ron Dabora Sergio D. Servetto arxiv:s/0505032v3 [s.it] 1 Nov 2006 Abstrat We onsider

More information

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum

More information

1 sin 2 r = 1 n 2 sin 2 i

1 sin 2 r = 1 n 2 sin 2 i Physis 505 Fall 005 Homework Assignment #11 Solutions Textbook problems: Ch. 7: 7.3, 7.5, 7.8, 7.16 7.3 Two plane semi-infinite slabs of the same uniform, isotropi, nonpermeable, lossless dieletri with

More information

Parallel Additive Gaussian Channels

Parallel Additive Gaussian Channels Parallel Additive Gaussian Channels Let us assume that we have N parallel one-dimensional channels disturbed by noise sources with variances σ 2,,σ 2 N. N 0,σ 2 x x N N 0,σ 2 N y y N Energy Constraint:

More information

3 Tidal systems modelling: ASMITA model

3 Tidal systems modelling: ASMITA model 3 Tidal systems modelling: ASMITA model 3.1 Introdution For many pratial appliations, simulation and predition of oastal behaviour (morphologial development of shorefae, beahes and dunes) at a ertain level

More information

max min z i i=1 x j k s.t. j=1 x j j:i T j

max min z i i=1 x j k s.t. j=1 x j j:i T j AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be

More information

9 Geophysics and Radio-Astronomy: VLBI VeryLongBaseInterferometry

9 Geophysics and Radio-Astronomy: VLBI VeryLongBaseInterferometry 9 Geophysis and Radio-Astronomy: VLBI VeryLongBaseInterferometry VLBI is an interferometry tehnique used in radio astronomy, in whih two or more signals, oming from the same astronomial objet, are reeived

More information

Determination of the reaction order

Determination of the reaction order 5/7/07 A quote of the wee (or amel of the wee): Apply yourself. Get all the eduation you an, but then... do something. Don't just stand there, mae it happen. Lee Iaoa Physial Chemistry GTM/5 reation order

More information

SOA/CAS MAY 2003 COURSE 1 EXAM SOLUTIONS

SOA/CAS MAY 2003 COURSE 1 EXAM SOLUTIONS SOA/CAS MAY 2003 COURSE 1 EXAM SOLUTIONS Prepared by S. Broverman e-mail 2brove@rogers.om website http://members.rogers.om/2brove 1. We identify the following events:. - wathed gymnastis, ) - wathed baseball,

More information

A simple expression for radial distribution functions of pure fluids and mixtures

A simple expression for radial distribution functions of pure fluids and mixtures A simple expression for radial distribution funtions of pure fluids and mixtures Enrio Matteoli a) Istituto di Chimia Quantistia ed Energetia Moleolare, CNR, Via Risorgimento, 35, 56126 Pisa, Italy G.

More information

arxiv:gr-qc/ v2 6 Feb 2004

arxiv:gr-qc/ v2 6 Feb 2004 Hubble Red Shift and the Anomalous Aeleration of Pioneer 0 and arxiv:gr-q/0402024v2 6 Feb 2004 Kostadin Trenčevski Faulty of Natural Sienes and Mathematis, P.O.Box 62, 000 Skopje, Maedonia Abstrat It this

More information

Diversity-Multiplexing Tradeoff in MIMO Channels with Partial CSIT. ECE 559 Presentation Hoa Pham Dec 3, 2007

Diversity-Multiplexing Tradeoff in MIMO Channels with Partial CSIT. ECE 559 Presentation Hoa Pham Dec 3, 2007 Diversity-Multiplexing Tradeoff in MIMO Channels with Partial CSIT ECE 559 Presentation Hoa Pham Dec 3, 2007 Introduction MIMO systems provide two types of gains Diversity Gain: each path from a transmitter

More information

On the Designs and Challenges of Practical Binary Dirty Paper Coding

On the Designs and Challenges of Practical Binary Dirty Paper Coding On the Designs and Challenges of Pratial Binary Dirty Paper Coding 04 / 08 / 2009 Gyu Bum Kyung and Chih-Chun Wang Center for Wireless Systems and Appliations Shool of Eletrial and Computer Eng. Outline

More information

ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION. Dobromir P. Kralchev

ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION. Dobromir P. Kralchev Pliska Stud. Math. Bulgar. 8 2007, 83 94 STUDIA MATHEMATICA BULGARICA ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION Dobromir P. Kralhev Consider the probability that the Brownian motion

More information

Counting Idempotent Relations

Counting Idempotent Relations Counting Idempotent Relations Beriht-Nr. 2008-15 Florian Kammüller ISSN 1436-9915 2 Abstrat This artile introdues and motivates idempotent relations. It summarizes haraterizations of idempotents and their

More information

Combined Electric and Magnetic Dipoles for Mesoband Radiation, Part 2

Combined Electric and Magnetic Dipoles for Mesoband Radiation, Part 2 Sensor and Simulation Notes Note 53 3 May 8 Combined Eletri and Magneti Dipoles for Mesoband Radiation, Part Carl E. Baum University of New Mexio Department of Eletrial and Computer Engineering Albuquerque

More information

Multi-version Coding for Consistent Distributed Storage of Correlated Data Updates

Multi-version Coding for Consistent Distributed Storage of Correlated Data Updates Multi-version Coding for Consistent Distributed Storage of Correlated Data Updates Ramy E. Ali and Vivek R. Cadambe 1 arxiv:1708.06042v1 [s.it] 21 Aug 2017 Abstrat Motivated by appliations of distributed

More information

Resolving RIPS Measurement Ambiguity in Maximum Likelihood Estimation

Resolving RIPS Measurement Ambiguity in Maximum Likelihood Estimation 14th International Conferene on Information Fusion Chiago, Illinois, USA, July 5-8, 011 Resolving RIPS Measurement Ambiguity in Maximum Likelihood Estimation Wenhao Li, Xuezhi Wang, and Bill Moran Shool

More information

arxiv:math/ v4 [math.ca] 29 Jul 2006

arxiv:math/ v4 [math.ca] 29 Jul 2006 arxiv:math/0109v4 [math.ca] 9 Jul 006 Contiguous relations of hypergeometri series Raimundas Vidūnas University of Amsterdam Abstrat The 15 Gauss ontiguous relations for F 1 hypergeometri series imply

More information

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena Page 1 of 10 Physial Laws, Absolutes, Relative Absolutes and Relativisti Time Phenomena Antonio Ruggeri modexp@iafria.om Sine in the field of knowledge we deal with absolutes, there are absolute laws that

More information

Average Rate Speed Scaling

Average Rate Speed Scaling Average Rate Speed Saling Nikhil Bansal David P. Bunde Ho-Leung Chan Kirk Pruhs May 2, 2008 Abstrat Speed saling is a power management tehnique that involves dynamially hanging the speed of a proessor.

More information

Probabilistic Graphical Models

Probabilistic Graphical Models Probabilisti Graphial Models David Sontag New York University Leture 12, April 19, 2012 Aknowledgement: Partially based on slides by Eri Xing at CMU and Andrew MCallum at UMass Amherst David Sontag (NYU)

More information

Ayan Kumar Bandyopadhyay

Ayan Kumar Bandyopadhyay Charaterization of radiating apertures using Multiple Multipole Method And Modeling and Optimization of a Spiral Antenna for Ground Penetrating Radar Appliations Ayan Kumar Bandyopadhyay FET-IESK, Otto-von-Guerike-University,

More information

Reliability Guaranteed Energy-Aware Frame-Based Task Set Execution Strategy for Hard Real-Time Systems

Reliability Guaranteed Energy-Aware Frame-Based Task Set Execution Strategy for Hard Real-Time Systems Reliability Guaranteed Energy-Aware Frame-Based ask Set Exeution Strategy for Hard Real-ime Systems Zheng Li a, Li Wang a, Shuhui Li a, Shangping Ren a, Gang Quan b a Illinois Institute of ehnology, Chiago,

More information

DESIGN FOR DIGITAL COMMUNICATION SYSTEMS VIA SAMPLED-DATA H CONTROL

DESIGN FOR DIGITAL COMMUNICATION SYSTEMS VIA SAMPLED-DATA H CONTROL DESIG FOR DIGITAL COMMUICATIO SYSTEMS VIA SAMPLED-DATA H COTROL M agahara 1 Y Yamamoto 2 Department of Applied Analysis and Complex Dynamial Systems Graduate Shool of Informatis Kyoto University Kyoto

More information

Likelihood-confidence intervals for quantiles in Extreme Value Distributions

Likelihood-confidence intervals for quantiles in Extreme Value Distributions Likelihood-onfidene intervals for quantiles in Extreme Value Distributions A. Bolívar, E. Díaz-Franés, J. Ortega, and E. Vilhis. Centro de Investigaión en Matemátias; A.P. 42, Guanajuato, Gto. 36; Méxio

More information

Ergodic and Outage Capacity of Narrowband MIMO Gaussian Channels

Ergodic and Outage Capacity of Narrowband MIMO Gaussian Channels Ergodic and Outage Capacity of Narrowband MIMO Gaussian Channels Yang Wen Liang Department of Electrical and Computer Engineering The University of British Columbia April 19th, 005 Outline of Presentation

More information

UPPER-TRUNCATED POWER LAW DISTRIBUTIONS

UPPER-TRUNCATED POWER LAW DISTRIBUTIONS Fratals, Vol. 9, No. (00) 09 World Sientifi Publishing Company UPPER-TRUNCATED POWER LAW DISTRIBUTIONS STEPHEN M. BURROUGHS and SARAH F. TEBBENS College of Marine Siene, University of South Florida, St.

More information