Parametrization of the Local Scattering Function Estimator for Vehicular-to-Vehicular Channels

Size: px
Start display at page:

Download "Parametrization of the Local Scattering Function Estimator for Vehicular-to-Vehicular Channels"

Transcription

1 Parametrization o the Local Scattering Function Estimator or Vehicular-to-Vehicular Channels Laura Bernadó, Thomas Zemen, Alexander Paier, ohan Karedal and Bernard H Fleury Forschungszentrum Teleommuniation Wien (tw), Vienna, Austria nstitut ür Nachrichtentechni und Hochrequenztechni, Technische Universität Wien, Vienna, Austria Department o Electrical and normation Technology, Lund University, Sweden Department o Electronics Systems, Aalborg University, Denmar contact: bernado@twat Abstract Non wide-sense stationary (WSS) uncorrelatedscatterering (US) ading processes are observed in vehicular communications To estimate such a process under additive white Gaussian noise we use the local scattering unction (LSF) n this paper we present an optimal parametrization o the multitaperbased LSF estimator We do this by quantizing the mean square error (MSE) For that purpose we use the structure o a twodimensional Wiener ilter and optimize the parameters o the estimator to obtain the minimum MSE (MMSE) We split the observed ading process in WSS regions and analyze the inluence o the estimator parameters and the length o the stationarity regions on the MMSE The analysis is perormed considering three dierent scenarios representing dierent scattering properties We show that there is an optimal combination o estimator parameters and length o stationarity region which provides a minimum MMSE NTRODUCTON n vehicular communications the ading process does not ulill the wide-sense stationary (WSS) uncorrelated-scattering (US) property Methods have been proposed to deal with non- WSSUS processes by repeating the experiment and perorming the second-order statistics calculation in the sample domain instead o the temporal domain [] n reality it is very diicult to obtain dierent realizations o the same experiment, while eeping the same experimental conditions Thereore we use the idea o splitting an observed process in small regions, in which we can assume that the WSSUS property holds [] n [] the length o these stationarity regions is assessed by means o the collinearity measure without optimizing the estimator parameters n [] an analysis o the estimator parameters is done or pedestrian mobility n this paper we compute the optimal parametrization o the LSF estimator or vehicular scenarios We minimize the mean square error (MSE) taing into account the length o the WSSUS region Contributions o the Paper The objective o the paper is to characterize the properties o the local scattering unction (LSF) estimator introduced in [] The estimator which is used to calculate the scattering unction This research was supported by the EC under the FP Networ o Excellence projects NEWCOM, as well as the project COCOMNT unded by Vienna Science and Technology Fund (WWTF) The Telecommunications Research Center Vienna (tw) is supported by the Austrian Government and the City o Vienna within the competence center program COMET o non-stationary processes n order to assess the perormance o the estimator, we deine the MSE based on the structure o a two-dimensional time-requency Wiener ilter [] We show that the Wiener ilter coeicients can be calculated rom the LSF t is noteworthy to mention that we do not use the Wiener ilter or iltering a signal, but or characterizing the perormance o an estimator Furthermore, we assess the length o the WSSUS region by means o the minimum MSE (MMSE) Notation Time t, requency, delay τ and Doppler shit ν are discrete variables Organization o the Paper n Section we introduce the two-dimensional (D) Wiener Filter concept to calculate the MSE o the estimator n Section the relation between the LSF and the ilter coeicients is deined The calculation o the ilter coeicients and their optimization, ie the choice o the estimator parameters which minimizes the MSE, are analyzed in Sections V and V respectively Conclusions are presented in Section V D WENER FLTER We want to optimize the parameters o the LSF estimator n order to do that, we use a D time-requency Wiener ilter described in Fig [] We consider a signal R(t, ) to be iltered which consists o the true channel transer unction H(t, ) corrupted with additive noise N(t, ) The optimum LSF parameter set minimizes the MSE between the output o the ilter Ĥ(t, ) and H(t, ) R(t, ) = H(t, )N(t, ) Fig D WENER FLTER H (t, ) D Wiener ilter scheme H(t, ) The estimated transer unction at the ilter output reads Ĥ(t, ) = M i= N j= - e(t, ) a i,j R(t i, j) ()

2 where a i,j are the ilter coeicients and M and N denote the length o the sequence R(t, ) in time and requency respectively The MSE is given by where E = E{ e(t, ) } e(t, ) =H(t, ) Ĥ(t, ) and E{} denotes expectation n order to ind the coeicients o this D ilter, we use the orthogonality principle E{e(t, )Ĥ (t, )} = to obtain the Wiener-Hop equation E{H(t, )R (t, )} = a(t,, t, ) t, E{R(t, )R (t, )} () We assume that the noise N(t, ) is a zero-mean process statistically independent o the channel requency response H(t, ) Under this assumption we can rewrite () as E{H(t, )H (t, )} = t, a(t,, t, ) E{R(t, )R (t, )} () From () we see that E{H(t, )H (t, )} is the timerequency (TF) auto-correlation unction (ACF) o H(t, ) Similarly, E{R(t, )R (t, )} is the TF-ACF o R(t, ) For short we rename these two TF-ACFs as R H and R R n order to deine the Wiener ilter, we must assume to have stationary processes, thereore the TF-ACFs will depend only on the time and requency lags and can be expressed as R H ( t, ) and R R ( t, ) For the sae o simplicity, we use the compact notation or (): R H = AR R From this identity we obtain the coeicients o the D Wiener ilter: A T = R T HR R () with R R = R R ( t, ) R R ( t, N ) R H R ( t, N ) R R( t, ), where R R (, ) R R (M, ) R R ( t, ) = RR (M, ) R R(, ) n the above expressions, () H denotes Hermitian transposition and () complex conjugation The matrix R H ollows the same structure, whereas A stems rom rewriting () in matrix notation, ie ĥ = A T r, where the vectors ĥ and r are the channel transer unction and its noisy version respectively: ĥ() Ĥ(, ) ĥ = with ĥ() = ĥ(m ) Ĥ(,N ) and r = r() r(m ) with r() = R(, ) R(,N ) FLTER MPLEMENTATON The TF ilter in () can be written as the D TF-convolution Ĥ(t, ) =a(t, ) R(t, ) () with a(t, ) denoting the ilter coeicients deined in () Perorming the Fourier transorm in both dimensions, we can express () as F t F {Ĥ(t, ) } = F t F {a(t, ) R(t, )} () SĤ(ν, τ) = A(ν, τ)s R (ν, τ), where SĤ(ν, τ) and S R (ν, τ) are the Doppler-delay spreading unctions o Ĥ(t, ) and R(t, ) n () F and F denote the Fourier transorm and its inverse respectively The ilter coeicients A(ν, τ) in () are given by A(ν, τ) =F t F { RH ( t, ) R R ( t, ) } = S H(ν, τ) S R (ν, τ) = C H(ν, τ) C R (ν, τ) with C H (ν, τ) and C R (ν, τ) denoting the Doppler-delay scattering unctions o H(t, ) and R(t, ) respectively n order to obtain Ĥ(t, ) we only need to reverse the sequence o Fourier transorms perormed in () at the output o the ilter V CALCULATON OF THE FLTER COEFFCENTS The ilter coeicients determined in () depend on the scattering unctions C R (ν, τ) and C H (ν, τ) We calculate them using a multitaper estimator in which the windows are chosen to be the discrete prolate spheroidal sequences (DPSS) [] Since we are dealing with non-wss processes, the observed process at the input o the ilter is divided in time regions over which we can assume that the WSS property holds This allows us to calculate the second-order moments o the process and, consequently, the ilter coeicients The estimate o C H (ν, τ) reads Ĉ H(ν, τ) = () L H (Gl) (ν, τ) () l= The ranges o the variables τ and ν in () are {,, N } and { M/, M/ } respectively Moreover, and

3 are the number o tapers in time and requency respectively and H(t## t, ## ) t = M/ = N/ τ ) C R (ν,!) R (t,) LSF ESTMATOR H (t,) Calculation Coeicients C H (ν,!) Fig (b) S-b (Highway- m/h) (c) S-a (Rural- m/h) (d) S-b (Rural- m/h) e(t,) A (ν,!) WSS region (e) S-a (Urban- m/h) () S-b (Urban- m/h) Fig Normalized squared envelope o the channel response measured in the three investigated scenarios (a) S-a (Highway- m/h) H(t,) C H (ν, τ ) C R (ν, τ ) H (t,) D WENER FLTER () is the tapered version o H(t, ) and Gl (t##, ## )e jπ(νt τ ) are the DPSS time-requency tapers n () t { M } or each region Since everything taes place locally, the estimate o the scattering unction in () is named local scattering unction [], [] The ilter coeicients deined in () will be also local They are ed bac to the ilter ater the estimation procedure (Fig ) n order to show explicitly this locality, we introduce the superscript in the notation Note that the ilter coeicients are calculated rom estimated unctions, thereore we will use estimates o the ilter coeicients We use the sampled version o the LSF deined in [] The WSS region is inite with dimensions M in time and N in requency The local ilter coeicients are deined as R(t,) = H(t,)N(t,) Gl (t##, ## )e jπ(νt A (ν, τ ) =!! H (Gl ) (ν, τ ) = N/ M/ Calculation o the ilter coeicients or each WSS region Even though this solution is considered optimal or the Wiener-iltering problem, our estimation o the LSF orces us to perorm another optimization step n the estimator () there is an optimal number o windows in time and requency that reduces the overall MSE The number o windows is determined by the time-bandwidth product rom () Besides that, we can also optimize the length o the stationarity regions M V O PTMZATON OF THE PARAMETERS OF THE ESTMATOR Recent measurements have reported non-stationary channel responses or vehicle-to-vehicle propagation [], and we thereore mae use o such measurements to demonstrate a solution or the above optimization problem Further details regarding the measurements are ound in [] As observed in [], communications between vehicle with opposite driving directions experience the largest temporal variations We consider three such scenarios (transmitter and receiver move at the same speed): Scenario (S): Highway environment There is a strong line o sight (LOS) component with diuse components and some relecting paths Considered speeds: (a) m/h and (b) m/h Scenario (S): Rural environment There is a strong LOS component with diuse components but no additional paths Considered speeds: (a) m/h and (b) m/h Scenario (S): Urban environment There is a strong LOS component with large diuse contributions and additional paths created by relections coming rom near objects Considered speeds: (a) m/h and (b) m/h n scenario (highway) the delay spread is short and some contributions arrive at late delays n scenario (rural) the delay spread is longer with no urther contributions n scenario (urban) the largest delay spread is observed with lots o paths coming rom close relecting objects Figure shows the squared magnitude o the time-varying impulse responses measured in the three scenarios Since the measured channel transer unctions have a signal-to-noise ratio (SNR) o roughly, we consider these as the true

4 transer unctions H(t, ) Noise-corrupted transer unctions R(t, ) are created by adding random noise to H(t, ) such that an SNR o is achieved We use the sampled channel transer unction H(t, ) = H(t T rep, B/Q), where T rep = µs is the repetition time o the channel sounder, B = MHz is the measurement bandwidth and Q = is the number o requency bins The variables t and are continuous We consider a measurement run o s with { Q } and t { S }, where S = samples A Number o Time-Frequency Tapers (Choice o (, )): n a irst step we select a given stationarity length M and optimize the parameters and For this irst analysis we set M = The choice o the time-bandwidth product determines the number o tapers used in the estimation process []: <N t W t in the time domain and <N W in the requency domain, where N t W t = i/ t and N W = j/ τ (N t W t = i and N W = j when using normalized t and τ) Our optimization problem is thus to solve ( ) E argmin, K The term to be optimized is the mean o the MSE per region, computed over a total number o K WSS regions The MSE per region is deined as E = MN M t= = N H (t, ) Ĥ (t, ) with < i, < j, and M, N denoting the extent o the WSS region We evaluate the MSE or all possible combinations o and rom to The resulting MSEs or all scenarios are plotted in Fig versus and using the gray-scale code reported on the right We highlight the minimum MSE with a red square at the pair (, ) which achieves it n each red square the value o the minimum scaled by is written As we can see in Fig, while increasing the number o tapers in both time and requency domains the MSE decreases rapidly and beyond a certain point starts to grow slowly This is due to the act that, by increasing the number o tapers, on one hand we reduce the variance, but on the other hand we increase the bias There is a trade-o between these two eects which corresponds to the best combination o the number o tapers in time and requency to minimize the MSE B Length o the Stationarity Region: The stationarity region is deined by two parameters: M (or the time domain) and N (or the requency domain) M has to be selected in order to ensure that the WSS property and N the US property When choosing M properly, we can also ensure that contributions at dierent delays are not correlated (they come rom dierent scatterers) We deine dierent regions with lengths M =,, and samples and calculate the MSE The length o this region is short enough to ensure (a) S-a (Highway- m/h) (c) S-a (Rural- m/h) (e) S-a (Urban- m/h) Fig x x x (b) S-b (Highway- m/h) (d) S-b (Rural- m/h) () S-b (Urban- m/h) MSE versus (, ) or the three dierent scenarios x x the US property to hold within one WSS region Although the optimization o the number o tapers was done previously in Sec V-A, here we analyze the dependency o the length o the stationarity region with the optimal (, ) pair Table reports the results plotted in Fig TABLE MMSE FOR THE OPTMAL (, ) COMBNATON FOR DFFERENT SCENAROS AND DFFERENT WSS REGON LENGTHS THE VALUES OF MMSE ARE SCALED BY S S S WSS region length M a (,)- (,)- (,)- (,)- b (,)- (,)- (,)- (,)- a (,)- (,)- (,)- (,)- b (,)- (,)- (,)- (,)- a (,)- (,)- (,)- (,)- b (,)- (,)- (,)- (,)- The MMSE has the same variation depending on M regardless o the scenario n Sec V-A we showed that there is an optimal parametrization which results in the minimum MSE (Fig ) n that case, the MSE gets smaller and then larger again while increasing the number o considered tapers in our estimator We observe a similar eect with the length o the stationarity region: when increasing the length o this region, the MMSE gets smaller and then grows again Figure depicts this result and shows that the increase is aster or x

5 higher speeds (S) Furthermore, when we increase the length o the WSS region, we observe a longer period o time and consequently more variations o the process Thus, we need to consider more windows in our multitaper estimator (Tab ) MMSE ( ) [linear scale] Fig Scenario Scenario Scenario a version b version M MMSE versus the WSS-region length or all scenarios n Fig, or a given scenario (we compare curves with the same color/marer), the achieved MMSE is smaller or the case (b), ie when the cars drive slower This shows the nonstationarity o the process and its relation to the MSE The less time-varying the channel is (the slower the cars drive), the smaller the achieved MMSE is We have to highlight the dierence between scenarios, even though all o them consider a strong LOS component Due to the speed o the cars it is clear that there are more time luctuations in scenario and results in the largest MMSE Even though the cars in scenario drive slower than in scenario it has a larger MMSE This is due to the large delay spread and numerous path contributions in scenario where we observe a more time-varying process So ar the presented results have been calculated with a SNR o n Fig we compare or scenario -a the MMSE or dierent SNRs o, and As expected, the pair (, ) achieving the MMSE depends on the length o the stationarity region This combination is written next to their corresponding MMSE value in Fig The MMSE decreases when SNR increases The shape o the curve is the same but shited upwards or downwards depending on the SNR The higher the SNR is, the lower the MMSE is V CONCLUSONS We assessed the perormance o the local scattering unction (LSF) by means o the mean square error (MSE) For that purpose we used a two-dimensional Wiener ilter We showed that there is a best parameters combination or the LSF which results in the minimum MSE (MMSE) and that the MSE decreases until it reaches a minimum and increases again when the number o tapers in the LSF increases The number o tapers achieving the MMSE increases when considering longer stationarity regions There is a length or which the MMSE is the minimum We chose the vehicular communications MMSE ( ) [linear scale] (,) (,) (,) (,) (,) (,) (,) (,) (,) SNR = SNR = SNR = (,) (,) (,) M Fig MMSE or S-a versus M or dierent SNRs environment to quantiy it and showed that, or a given scenario, the slower the cars drive, the smaller the MMSE is When comparing dierent scenarios, we showed that the MMSE depends on the non-stationarity o the environment The MMSE is smaller or more stationary scenarios n this sense, the highway scenario, due to the high speeds o the cars, is the most time-varying and the rural scenario is the least, given that it presents a short delay spread and no urther contributions Although the speeds o the cars in the urban scenario are the lowest, the scattering environment contributes to creating a long delay spread and thereore a more timevarying environment REFERENCES [] S Bendat and A G Piersol, Engineering Applications o Correlation and Spectral Analysis ohn Wiley & Sons, nc, [] G Matz, Doubly underspread non-wssus channels: Analysis and estimation o channel statistics, in Proc EEE nt Worshop on Signal Processing Advance Wireless Communications (SPAWC), Rome, taly, une, pp [] A Paier, T Zemen, L Bernadó, G Matz, Karedal, N Czin, C Dumard, F Tuvesson, A F Molisch, and C F Meclenbräuer, Non-WSSUS vehicular channel characterization in highway and urban scenarios at GHz using the local scattering unction, in Worshop on Smart Antennas (WSA), Darmstadt, Germany, February [] S Kaiser, Multi-carrier CDMA mobile radio systems-analysis and optimization o detection, decoding and channel estimation, PhD dissertation, German Aerospace Center (DLR) nstitute o Communications and Navigation, Germany, [] D Slepian, Prolate spheroidal wave unctions, Fourier analysis, and uncertainty - V: The discrete case, The Bell System Technical ournal, vol, no, pp, May-une [] G Matz, On non-wssus wireless ading channels, EEE Trans Wireless Commun, vol, no, pp, September [] L Bernadó, T Zemen, A Paier, G Matz, Karedal, N Czin, C Dumard, F Tuvesson, M Hagenauer, A F Molisch, and C F Meclenbräuer, Non-WSSUS vehicular channel characterization at GHz - spectral divergence and time-variant coherence parameters, in Proceedings o the XXXth URS General Assembly, Chicago, USA, August [] A Paier, Karedal, N Czin, H Hostetter, C Dumard, T Zemen, F Tuvesson, C F Meclenbräuer, and A F Molisch, First results rom car-to-car and car-to-inrastructure radio channel measurements at GHz, in nternational Symposium on Personal, ndoor and Mobile Radio Communications (PMRC ), September, pp [] D B Percival and A T Walden, Spectral Analysis or Physical Applications Cambridge University Press,

Spatial Diversity and Spatial Correlation Evaluation of Measured Vehicle-to-Vehicle Radio Channels at 5.2 GHZ

Spatial Diversity and Spatial Correlation Evaluation of Measured Vehicle-to-Vehicle Radio Channels at 5.2 GHZ MITSUBISHI ELECTRIC RESEARCH LABORATORIES http://www.merl.com Spatial Diversity and Spatial Correlation Evaluation of Measured Vehicle-to-Vehicle Radio Channels at 5. GHZ Alexander Paier, Thomas Zemen,

More information

Empirical Relationship between Local Scattering Function and Joint Probability Density Function

Empirical Relationship between Local Scattering Function and Joint Probability Density Function Empirical Relationship between Local Scattering Function and Joint Probability Density Function Michael Walter, Thomas Zemen and Dmitriy Shutin German Aerospace Center (DLR), Münchener Straße 2, 82234

More information

TLT-5200/5206 COMMUNICATION THEORY, Exercise 3, Fall TLT-5200/5206 COMMUNICATION THEORY, Exercise 3, Fall Problem 1.

TLT-5200/5206 COMMUNICATION THEORY, Exercise 3, Fall TLT-5200/5206 COMMUNICATION THEORY, Exercise 3, Fall Problem 1. TLT-5/56 COMMUNICATION THEORY, Exercise 3, Fall Problem. The "random walk" was modelled as a random sequence [ n] where W[i] are binary i.i.d. random variables with P[W[i] = s] = p (orward step with probability

More information

IN mobile communication systems channel state information

IN mobile communication systems channel state information 4534 IEEE TRANSACTIONS ON SIGNAL PROCESSING, VOL 55, NO 9, SEPTEMBER 2007 Minimum-Energy Band-Limited Predictor With Dynamic Subspace Selection for Time-Variant Flat-Fading Channels Thomas Zemen, Christoph

More information

Additional exercises in Stationary Stochastic Processes

Additional exercises in Stationary Stochastic Processes Mathematical Statistics, Centre or Mathematical Sciences Lund University Additional exercises 8 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *

More information

CHAPTER 8 ANALYSIS OF AVERAGE SQUARED DIFFERENCE SURFACES

CHAPTER 8 ANALYSIS OF AVERAGE SQUARED DIFFERENCE SURFACES CAPTER 8 ANALYSS O AVERAGE SQUARED DERENCE SURACES n Chapters 5, 6, and 7, the Spectral it algorithm was used to estimate both scatterer size and total attenuation rom the backscattered waveorms by minimizing

More information

LOW COMPLEXITY SIMULATION OF WIRELESS CHANNELS USING DISCRETE PROLATE SPHEROIDAL SEQUENCES

LOW COMPLEXITY SIMULATION OF WIRELESS CHANNELS USING DISCRETE PROLATE SPHEROIDAL SEQUENCES LOW COMPLEXITY SIMULATION OF WIRELESS CHANNELS USING DISCRETE PROLATE SPHEROIDAL SEQUENCES Florian Kaltenberger 1, Thomas Zemen 2, Christoph W. Ueberhuber 3 1 Corresponding Author: F. Kaltenberger ARC

More information

Lecture 2. Fading Channel

Lecture 2. Fading Channel 1 Lecture 2. Fading Channel Characteristics of Fading Channels Modeling of Fading Channels Discrete-time Input/Output Model 2 Radio Propagation in Free Space Speed: c = 299,792,458 m/s Isotropic Received

More information

Asymptotic Capacity Results for Non-Stationary Time-Variant Channels Using Subspace Projections

Asymptotic Capacity Results for Non-Stationary Time-Variant Channels Using Subspace Projections IEEE TRANSACTIONS ON INFORMATION THEORY, SUBMITTED (MAY 10, 2005). 1 Asymptotic Capacity Results for Non-Stationary Time-Variant Channels Using Subspace Projections arxiv:cs.it/0505020 v1 10 May 2005 Thomas

More information

Lecture 13: Applications of Fourier transforms (Recipes, Chapter 13)

Lecture 13: Applications of Fourier transforms (Recipes, Chapter 13) Lecture 13: Applications o Fourier transorms (Recipes, Chapter 13 There are many applications o FT, some o which involve the convolution theorem (Recipes 13.1: The convolution o h(t and r(t is deined by

More information

Asymptotic Capacity Results for Non-Stationary Time-Variant Channels Using Subspace Projections

Asymptotic Capacity Results for Non-Stationary Time-Variant Channels Using Subspace Projections IEEE TRANSACTIONS ON INFORMATION THEORY, SUBMITTED (MAY 10, 2005). 1 Asymptotic Capacity Results for Non-Stationary Time-Variant Channels Using Subspace Projections arxiv:cs/0505020v1 [cs.it] 10 May 2005

More information

Figure 18: Top row: example of a purely continuous spectrum (left) and one realization

Figure 18: Top row: example of a purely continuous spectrum (left) and one realization 1..5 S(). -.2 -.5 -.25..25.5 64 128 64 128 16 32 requency time time Lag 1..5 S(). -.5-1. -.5 -.1.1.5 64 128 64 128 16 32 requency time time Lag Figure 18: Top row: example o a purely continuous spectrum

More information

Mixed Signal IC Design Notes set 6: Mathematics of Electrical Noise

Mixed Signal IC Design Notes set 6: Mathematics of Electrical Noise ECE45C /8C notes, M. odwell, copyrighted 007 Mied Signal IC Design Notes set 6: Mathematics o Electrical Noise Mark odwell University o Caliornia, Santa Barbara rodwell@ece.ucsb.edu 805-893-344, 805-893-36

More information

ENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University

ENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University ENSC37 Communications Systems : Fourier Representations School o Engineering Science Simon Fraser University Outline Chap..5: Signal Classiications Fourier Transorm Dirac Delta Function Unit Impulse Fourier

More information

SIO 211B, Rudnick. We start with a definition of the Fourier transform! ĝ f of a time series! ( )

SIO 211B, Rudnick. We start with a definition of the Fourier transform! ĝ f of a time series! ( ) SIO B, Rudnick! XVIII.Wavelets The goal o a wavelet transorm is a description o a time series that is both requency and time selective. The wavelet transorm can be contrasted with the well-known and very

More information

Estimation of Performance Loss Due to Delay in Channel Feedback in MIMO Systems

Estimation of Performance Loss Due to Delay in Channel Feedback in MIMO Systems MITSUBISHI ELECTRIC RESEARCH LABORATORIES http://www.merl.com Estimation of Performance Loss Due to Delay in Channel Feedback in MIMO Systems Jianxuan Du Ye Li Daqing Gu Andreas F. Molisch Jinyun Zhang

More information

3. ESTIMATION OF SIGNALS USING A LEAST SQUARES TECHNIQUE

3. ESTIMATION OF SIGNALS USING A LEAST SQUARES TECHNIQUE 3. ESTIMATION OF SIGNALS USING A LEAST SQUARES TECHNIQUE 3.0 INTRODUCTION The purpose of this chapter is to introduce estimators shortly. More elaborated courses on System Identification, which are given

More information

Notes on Wavelets- Sandra Chapman (MPAGS: Time series analysis) # $ ( ) = G f. y t

Notes on Wavelets- Sandra Chapman (MPAGS: Time series analysis) # $ ( ) = G f. y t Wavelets Recall: we can choose! t ) as basis on which we expand, ie: ) = y t ) = G! t ) y t! may be orthogonal chosen or appropriate properties. This is equivalent to the transorm: ) = G y t )!,t )d 2

More information

A Non-Stationary MIMO Vehicle-to-Vehicle Channel Model Based on the Geometrical T-Junction Model Ali Chelli and Matthias Pätzold

A Non-Stationary MIMO Vehicle-to-Vehicle Channel Model Based on the Geometrical T-Junction Model Ali Chelli and Matthias Pätzold A Non-Stationary MIMO Vehicle-to-Vehicle Channel Model Based on the Geometrical -Junction Model Ali Chelli and Matthias Pätzold Faculty of Engineering and Science, University of Agder Service Box 59, N-4898

More information

Asymptote. 2 Problems 2 Methods

Asymptote. 2 Problems 2 Methods Asymptote Problems Methods Problems Assume we have the ollowing transer unction which has a zero at =, a pole at = and a pole at =. We are going to look at two problems: problem is where >> and problem

More information

Two-step self-tuning phase-shifting interferometry

Two-step self-tuning phase-shifting interferometry Two-step sel-tuning phase-shiting intererometry J. Vargas, 1,* J. Antonio Quiroga, T. Belenguer, 1 M. Servín, 3 J. C. Estrada 3 1 Laboratorio de Instrumentación Espacial, Instituto Nacional de Técnica

More information

In many diverse fields physical data is collected or analysed as Fourier components.

In many diverse fields physical data is collected or analysed as Fourier components. 1. Fourier Methods In many diverse ields physical data is collected or analysed as Fourier components. In this section we briely discuss the mathematics o Fourier series and Fourier transorms. 1. Fourier

More information

CHARACTERIZATION AND ANALYSIS OF DOUBLY DISPERSIVE MIMO CHANNELS. Gerald Matz

CHARACTERIZATION AND ANALYSIS OF DOUBLY DISPERSIVE MIMO CHANNELS. Gerald Matz CHARACTERIZATION AND ANALYSIS OF DOUBLY DISPERSIVE MIMO CHANNELS Gerald Matz Institute of Communications and Radio-Frequency Engineering, Vienna University of Technology Gusshausstrasse 2/389, A-14 Vienna,

More information

Digital Image Processing. Lecture 6 (Enhancement) Bu-Ali Sina University Computer Engineering Dep. Fall 2009

Digital Image Processing. Lecture 6 (Enhancement) Bu-Ali Sina University Computer Engineering Dep. Fall 2009 Digital Image Processing Lecture 6 (Enhancement) Bu-Ali Sina University Computer Engineering Dep. Fall 009 Outline Image Enhancement in Spatial Domain Spatial Filtering Smoothing Filters Median Filter

More information

Signals & Linear Systems Analysis Chapter 2&3, Part II

Signals & Linear Systems Analysis Chapter 2&3, Part II Signals & Linear Systems Analysis Chapter &3, Part II Dr. Yun Q. Shi Dept o Electrical & Computer Engr. New Jersey Institute o echnology Email: shi@njit.edu et used or the course:

More information

Unbiased Power Prediction of Rayleigh Fading Channels

Unbiased Power Prediction of Rayleigh Fading Channels Unbiased Power Prediction of Rayleigh Fading Channels Torbjörn Ekman UniK PO Box 70, N-2027 Kjeller, Norway Email: torbjorn.ekman@signal.uu.se Mikael Sternad and Anders Ahlén Signals and Systems, Uppsala

More information

IMPROVED NOISE CANCELLATION IN DISCRETE COSINE TRANSFORM DOMAIN USING ADAPTIVE BLOCK LMS FILTER

IMPROVED NOISE CANCELLATION IN DISCRETE COSINE TRANSFORM DOMAIN USING ADAPTIVE BLOCK LMS FILTER SANJAY KUMAR GUPTA* et al. ISSN: 50 3676 [IJESAT] INTERNATIONAL JOURNAL OF ENGINEERING SCIENCE & ADVANCED TECHNOLOGY Volume-, Issue-3, 498 50 IMPROVED NOISE CANCELLATION IN DISCRETE COSINE TRANSFORM DOMAIN

More information

SPOC: An Innovative Beamforming Method

SPOC: An Innovative Beamforming Method SPOC: An Innovative Beamorming Method Benjamin Shapo General Dynamics Ann Arbor, MI ben.shapo@gd-ais.com Roy Bethel The MITRE Corporation McLean, VA rbethel@mitre.org ABSTRACT The purpose o a radar or

More information

Analog Communication (10EC53)

Analog Communication (10EC53) UNIT-1: RANDOM PROCESS: Random variables: Several random variables. Statistical averages: Function o Random variables, moments, Mean, Correlation and Covariance unction: Principles o autocorrelation unction,

More information

2 Frequency-Domain Analysis

2 Frequency-Domain Analysis 2 requency-domain Analysis Electrical engineers live in the two worlds, so to speak, o time and requency. requency-domain analysis is an extremely valuable tool to the communications engineer, more so

More information

Fading Statistical description of the wireless channel

Fading Statistical description of the wireless channel Channel Modelling ETIM10 Lecture no: 3 Fading Statistical description of the wireless channel Fredrik Tufvesson Department of Electrical and Information Technology Lund University, Sweden Fredrik.Tufvesson@eit.lth.se

More information

Multiple Antennas. Mats Bengtsson, Björn Ottersten. Channel characterization and modeling 1 September 8, Signal KTH Research Focus

Multiple Antennas. Mats Bengtsson, Björn Ottersten. Channel characterization and modeling 1 September 8, Signal KTH Research Focus Multiple Antennas Channel Characterization and Modeling Mats Bengtsson, Björn Ottersten Channel characterization and modeling 1 September 8, 2005 Signal Processing @ KTH Research Focus Channel modeling

More information

VIII. Coherence and Transfer Function Applications A. Coherence Function Estimates

VIII. Coherence and Transfer Function Applications A. Coherence Function Estimates VIII. Coherence and Transfer Function Applications A. Coherence Function Estimates Consider the application of these ideas to the specific problem of atmospheric turbulence measurements outlined in Figure

More information

Maximum Achievable Diversity for MIMO-OFDM Systems with Arbitrary. Spatial Correlation

Maximum Achievable Diversity for MIMO-OFDM Systems with Arbitrary. Spatial Correlation Maximum Achievable Diversity for MIMO-OFDM Systems with Arbitrary Spatial Correlation Ahmed K Sadek, Weifeng Su, and K J Ray Liu Department of Electrical and Computer Engineering, and Institute for Systems

More information

Scattered Data Approximation of Noisy Data via Iterated Moving Least Squares

Scattered Data Approximation of Noisy Data via Iterated Moving Least Squares Scattered Data Approximation o Noisy Data via Iterated Moving Least Squares Gregory E. Fasshauer and Jack G. Zhang Abstract. In this paper we ocus on two methods or multivariate approximation problems

More information

NOISE ROBUST RELATIVE TRANSFER FUNCTION ESTIMATION. M. Schwab, P. Noll, and T. Sikora. Technical University Berlin, Germany Communication System Group

NOISE ROBUST RELATIVE TRANSFER FUNCTION ESTIMATION. M. Schwab, P. Noll, and T. Sikora. Technical University Berlin, Germany Communication System Group NOISE ROBUST RELATIVE TRANSFER FUNCTION ESTIMATION M. Schwab, P. Noll, and T. Sikora Technical University Berlin, Germany Communication System Group Einsteinufer 17, 1557 Berlin (Germany) {schwab noll

More information

Implementation of a Space-Time-Channel-Filter

Implementation of a Space-Time-Channel-Filter Implementation of a Space-Time-Channel-Filter Nadja Lohse, Clemens Michalke, Marcus Bronzel and Gerhard Fettweis Dresden University of Technology Mannesmann Mobilfunk Chair for Mobile Communications Systems

More information

Least-Squares Spectral Analysis Theory Summary

Least-Squares Spectral Analysis Theory Summary Least-Squares Spectral Analysis Theory Summary Reerence: Mtamakaya, J. D. (2012). Assessment o Atmospheric Pressure Loading on the International GNSS REPRO1 Solutions Periodic Signatures. Ph.D. dissertation,

More information

Communications and Signal Processing Spring 2017 MSE Exam

Communications and Signal Processing Spring 2017 MSE Exam Communications and Signal Processing Spring 2017 MSE Exam Please obtain your Test ID from the following table. You must write your Test ID and name on each of the pages of this exam. A page with missing

More information

A Systematic Approach to Frequency Compensation of the Voltage Loop in Boost PFC Pre- regulators.

A Systematic Approach to Frequency Compensation of the Voltage Loop in Boost PFC Pre- regulators. A Systematic Approach to Frequency Compensation o the Voltage Loop in oost PFC Pre- regulators. Claudio Adragna, STMicroelectronics, Italy Abstract Venable s -actor method is a systematic procedure that

More information

Introduction to Analog And Digital Communications

Introduction to Analog And Digital Communications Introduction to Analog And Digital Communications Second Edition Simon Haykin, Michael Moher Chapter Fourier Representation o Signals and Systems.1 The Fourier Transorm. Properties o the Fourier Transorm.3

More information

Lab 3: The FFT and Digital Filtering. Slides prepared by: Chun-Te (Randy) Chu

Lab 3: The FFT and Digital Filtering. Slides prepared by: Chun-Te (Randy) Chu Lab 3: The FFT and Digital Filtering Slides prepared by: Chun-Te (Randy) Chu Lab 3: The FFT and Digital Filtering Assignment 1 Assignment 2 Assignment 3 Assignment 4 Assignment 5 What you will learn in

More information

Probabilistic Analysis of Multi-layered Soil Effects on Shallow Foundation Settlement

Probabilistic Analysis of Multi-layered Soil Effects on Shallow Foundation Settlement Probabilistic Analysis o Multi-layered Soil ects on Shallow Foundation Settlement 54 Y L Kuo B Postgraduate Student, School o Civil and nvironmental ngineering, University o Adelaide, Australia M B Jaksa

More information

UNCERTAINTY EVALUATION OF SINUSOIDAL FORCE MEASUREMENT

UNCERTAINTY EVALUATION OF SINUSOIDAL FORCE MEASUREMENT XXI IMEKO World Congress Measurement in Research and Industry August 30 eptember 4, 05, Prague, Czech Republic UNCERTAINTY EVALUATION OF INUOIDAL FORCE MEAUREMENT Christian chlegel, Gabriela Kiekenap,Rol

More information

Mobile Radio Communications

Mobile Radio Communications Course 3: Radio wave propagation Session 3, page 1 Propagation mechanisms free space propagation reflection diffraction scattering LARGE SCALE: average attenuation SMALL SCALE: short-term variations in

More information

Treatment and analysis of data Applied statistics Lecture 6: Bayesian estimation

Treatment and analysis of data Applied statistics Lecture 6: Bayesian estimation Treatment and analysis o data Applied statistics Lecture 6: Bayesian estimation Topics covered: Bayes' Theorem again Relation to Likelihood Transormation o pd A trivial example Wiener ilter Malmquist bias

More information

A Simple Stochastic Channel Simulator for Car-to-Car Communication at 24 GHz

A Simple Stochastic Channel Simulator for Car-to-Car Communication at 24 GHz A Simple Stochastic Channel Simulator for Car-to-Car Communication at 24 GHz Micha Linde, Communications Engineering Lab (CEL), Karlsruhe Institute of Technology (KIT), Germany micha.linde@student.kit.edu

More information

Comparative Analysis of Equalization Methods for SC-FDMA

Comparative Analysis of Equalization Methods for SC-FDMA Comparative Analysis of Equalization Methods for SC-MA Anton ogadaev, Alexander Kozlov SUA Russia Email: {dak, akozlov}@vu.spb.ru Ann Ukhanova U otonik enmark Email: annuk@fotonik.dtu.dk Abstract n this

More information

9.1 The Square Root Function

9.1 The Square Root Function Section 9.1 The Square Root Function 869 9.1 The Square Root Function In this section we turn our attention to the square root unction, the unction deined b the equation () =. (1) We begin the section

More information

The achievable limits of operational modal analysis. * Siu-Kui Au 1)

The achievable limits of operational modal analysis. * Siu-Kui Au 1) The achievable limits o operational modal analysis * Siu-Kui Au 1) 1) Center or Engineering Dynamics and Institute or Risk and Uncertainty, University o Liverpool, Liverpool L69 3GH, United Kingdom 1)

More information

Systems & Signals 315

Systems & Signals 315 1 / 15 Systems & Signals 315 Lecture 13: Signals and Linear Systems Dr. Herman A. Engelbrecht Stellenbosch University Dept. E & E Engineering 2 Maart 2009 Outline 2 / 15 1 Signal Transmission through a

More information

Lecture 7: Wireless Channels and Diversity Advanced Digital Communications (EQ2410) 1

Lecture 7: Wireless Channels and Diversity Advanced Digital Communications (EQ2410) 1 Wireless : Wireless Advanced Digital Communications (EQ2410) 1 Thursday, Feb. 11, 2016 10:00-12:00, B24 1 Textbook: U. Madhow, Fundamentals of Digital Communications, 2008 1 / 15 Wireless Lecture 1-6 Equalization

More information

References Ideal Nyquist Channel and Raised Cosine Spectrum Chapter 4.5, 4.11, S. Haykin, Communication Systems, Wiley.

References Ideal Nyquist Channel and Raised Cosine Spectrum Chapter 4.5, 4.11, S. Haykin, Communication Systems, Wiley. Baseand Data Transmission III Reerences Ideal yquist Channel and Raised Cosine Spectrum Chapter 4.5, 4., S. Haykin, Communication Systems, iley. Equalization Chapter 9., F. G. Stremler, Communication Systems,

More information

Estimation of the Optimum Rotational Parameter for the Fractional Fourier Transform Using Domain Decomposition

Estimation of the Optimum Rotational Parameter for the Fractional Fourier Transform Using Domain Decomposition Estimation of the Optimum Rotational Parameter for the Fractional Fourier Transform Using Domain Decomposition Seema Sud 1 1 The Aerospace Corporation, 4851 Stonecroft Blvd. Chantilly, VA 20151 Abstract

More information

Predicting CSI for Link Adaptation Employing Support Vector Regression for Channel Extrapolation

Predicting CSI for Link Adaptation Employing Support Vector Regression for Channel Extrapolation Predicting CSI for Lin Adaptation Employing Support Vector Regression for Channel Extrapolation Allaeddine Djouama, Erich Zöchmann, Stefan Pratschner, Marus Rupp, Fatiha Youcef Ettoumi Department of Electronic

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 3 Signals & Systems Pro. Mark Fowler Discussion #9 Illustrating the Errors in DFT Processing DFT or Sonar Processing Example # Illustrating The Errors in DFT Processing Illustrating the Errors in

More information

ECE6604 PERSONAL & MOBILE COMMUNICATIONS. Week 3. Flat Fading Channels Envelope Distribution Autocorrelation of a Random Process

ECE6604 PERSONAL & MOBILE COMMUNICATIONS. Week 3. Flat Fading Channels Envelope Distribution Autocorrelation of a Random Process 1 ECE6604 PERSONAL & MOBILE COMMUNICATIONS Week 3 Flat Fading Channels Envelope Distribution Autocorrelation of a Random Process 2 Multipath-Fading Mechanism local scatterers mobile subscriber base station

More information

Random Error Analysis of Inertial Sensors output Based on Allan Variance Shaochen Li1, a, Xiaojing Du2,b and Junyi Zhai3,c

Random Error Analysis of Inertial Sensors output Based on Allan Variance Shaochen Li1, a, Xiaojing Du2,b and Junyi Zhai3,c International Conerence on Civil, Transportation and Environment (ICCTE 06) Random Error Analysis o Inertial Sensors output Based on Allan Variance Shaochen Li, a, Xiaojing Du, and Junyi Zhai3,c School

More information

s o (t) = S(f)H(f; t)e j2πft df,

s o (t) = S(f)H(f; t)e j2πft df, Sample Problems for Midterm. The sample problems for the fourth and fifth quizzes as well as Example on Slide 8-37 and Example on Slides 8-39 4) will also be a key part of the second midterm.. For a causal)

More information

2. SPECTRAL ANALYSIS APPLIED TO STOCHASTIC PROCESSES

2. SPECTRAL ANALYSIS APPLIED TO STOCHASTIC PROCESSES 2. SPECTRAL ANALYSIS APPLIED TO STOCHASTIC PROCESSES 2.0 THEOREM OF WIENER- KHINTCHINE An important technique in the study of deterministic signals consists in using harmonic functions to gain the spectral

More information

MIMO Signal Description for Spatial-Variant Filter Generation

MIMO Signal Description for Spatial-Variant Filter Generation MIMO Signal Description for Spatial-Variant Filter Generation Nadja Lohse and Marcus Bronzel and Gerhard Fettweis Abstract: Channel modelling today has to address time-variant systems with multiple antennas

More information

Physics 5153 Classical Mechanics. Solution by Quadrature-1

Physics 5153 Classical Mechanics. Solution by Quadrature-1 October 14, 003 11:47:49 1 Introduction Physics 5153 Classical Mechanics Solution by Quadrature In the previous lectures, we have reduced the number o eective degrees o reedom that are needed to solve

More information

Signals and Spectra - Review

Signals and Spectra - Review Signals and Spectra - Review SIGNALS DETERMINISTIC No uncertainty w.r.t. the value of a signal at any time Modeled by mathematical epressions RANDOM some degree of uncertainty before the signal occurs

More information

Statistical characterization of non-wssus mobile radio channels

Statistical characterization of non-wssus mobile radio channels originalarbeiten Statistical characterization of non-wssus mobile radio channels G. MATZ OVE IEEE Dedicated to Univ.-Prof. Dr. Ernst Bonek, on the occasion of his retirement. In this paper, statistical

More information

Evaluation of Suburban measurements by eigenvalue statistics

Evaluation of Suburban measurements by eigenvalue statistics Evaluation of Suburban measurements by eigenvalue statistics Helmut Hofstetter, Ingo Viering, Wolfgang Utschick Forschungszentrum Telekommunikation Wien, Donau-City-Straße 1, 1220 Vienna, Austria. Siemens

More information

Ultra Fast Calculation of Temperature Profiles of VLSI ICs in Thermal Packages Considering Parameter Variations

Ultra Fast Calculation of Temperature Profiles of VLSI ICs in Thermal Packages Considering Parameter Variations Ultra Fast Calculation o Temperature Proiles o VLSI ICs in Thermal Packages Considering Parameter Variations Je-Hyoung Park, Virginia Martín Hériz, Ali Shakouri, and Sung-Mo Kang Dept. o Electrical Engineering,

More information

Perfect Modeling and Simulation of Measured Spatio-Temporal Wireless Channels

Perfect Modeling and Simulation of Measured Spatio-Temporal Wireless Channels Perfect Modeling and Simulation of Measured Spatio-Temporal Wireless Channels Matthias Pätzold Agder University College Faculty of Engineering and Science N-4876 Grimstad, Norway matthiaspaetzold@hiano

More information

INTRODUCTION Noise is present in many situations of daily life for ex: Microphones will record noise and speech. Goal: Reconstruct original signal Wie

INTRODUCTION Noise is present in many situations of daily life for ex: Microphones will record noise and speech. Goal: Reconstruct original signal Wie WIENER FILTERING Presented by N.Srikanth(Y8104060), M.Manikanta PhaniKumar(Y8104031). INDIAN INSTITUTE OF TECHNOLOGY KANPUR Electrical Engineering dept. INTRODUCTION Noise is present in many situations

More information

Stochastic Processes. A stochastic process is a function of two variables:

Stochastic Processes. A stochastic process is a function of two variables: Stochastic Processes Stochastic: from Greek stochastikos, proceeding by guesswork, literally, skillful in aiming. A stochastic process is simply a collection of random variables labelled by some parameter:

More information

Diversity-Fidelity Tradeoff in Transmission of Analog Sources over MIMO Fading Channels

Diversity-Fidelity Tradeoff in Transmission of Analog Sources over MIMO Fading Channels Diversity-Fidelity Tradeo in Transmission o Analog Sources over MIMO Fading Channels Mahmoud Taherzadeh, Kamyar Moshksar and Amir K. Khandani Coding & Signal Transmission Laboratory www.cst.uwaterloo.ca

More information

Time-Variant Channel Equalization via Discrete Prolate Spheroidal Sequences

Time-Variant Channel Equalization via Discrete Prolate Spheroidal Sequences Time-Variant Channel Equalization via Discrete Prolate Spheroidal Sequences Thomas Zemen and Christoph F. Mecklenbräuker Telecommunication Research Center Vienna (ftw.) Tech Gate Vienna, Donau-City Str.

More information

Advanced 3 G and 4 G Wireless Communication Prof. Aditya K Jagannathan Department of Electrical Engineering Indian Institute of Technology, Kanpur

Advanced 3 G and 4 G Wireless Communication Prof. Aditya K Jagannathan Department of Electrical Engineering Indian Institute of Technology, Kanpur Advanced 3 G and 4 G Wireless Communication Prof. Aditya K Jagannathan Department of Electrical Engineering Indian Institute of Technology, Kanpur Lecture - 19 Multi-User CDMA Uplink and Asynchronous CDMA

More information

12.4 Known Channel (Water-Filling Solution)

12.4 Known Channel (Water-Filling Solution) ECEn 665: Antennas and Propagation for Wireless Communications 54 2.4 Known Channel (Water-Filling Solution) The channel scenarios we have looed at above represent special cases for which the capacity

More information

Figure 3.1 Effect on frequency spectrum of increasing period T 0. Consider the amplitude spectrum of a periodic waveform as shown in Figure 3.2.

Figure 3.1 Effect on frequency spectrum of increasing period T 0. Consider the amplitude spectrum of a periodic waveform as shown in Figure 3.2. 3. Fourier ransorm From Fourier Series to Fourier ransorm [, 2] In communication systems, we oten deal with non-periodic signals. An extension o the time-requency relationship to a non-periodic signal

More information

Scattering of Solitons of Modified KdV Equation with Self-consistent Sources

Scattering of Solitons of Modified KdV Equation with Self-consistent Sources Commun. Theor. Phys. Beijing, China 49 8 pp. 89 84 c Chinese Physical Society Vol. 49, No. 4, April 5, 8 Scattering o Solitons o Modiied KdV Equation with Sel-consistent Sources ZHANG Da-Jun and WU Hua

More information

, the time-correlation function

, the time-correlation function 270 IEEE TRANSACTIONS ON VEHICULAR TECHNOLOGY, VOL. 47, NO. 1, FEBRUARY 1998 On the Correlation Scattering Functions of the WSSUS Channel for Mobile Communications John S. Sadowsky, Member, IEEE, Venceslav

More information

Improved Detected Data Processing for Decision-Directed Tracking of MIMO Channels

Improved Detected Data Processing for Decision-Directed Tracking of MIMO Channels Improved Detected Data Processing for Decision-Directed Tracking of MIMO Channels Emna Eitel and Joachim Speidel Institute of Telecommunications, University of Stuttgart, Germany Abstract This paper addresses

More information

A CORRELATION TENSOR BASED MODEL FOR TIME VARIANT FREQUENCY SELECTIVE MIMO CHANNELS. Martin Weis, Giovanni Del Galdo, and Martin Haardt

A CORRELATION TENSOR BASED MODEL FOR TIME VARIANT FREQUENCY SELECTIVE MIMO CHANNELS. Martin Weis, Giovanni Del Galdo, and Martin Haardt A CORRELATON TENSOR BASED MODEL FOR TME VARANT FREQUENCY SELECTVE MMO CHANNELS Martin Weis Giovanni Del Galdo and Martin Haardt lmenau University of Technology - Communications Research Laboratory P.O.

More information

ITERATED SRINKAGE ALGORITHM FOR BASIS PURSUIT MINIMIZATION

ITERATED SRINKAGE ALGORITHM FOR BASIS PURSUIT MINIMIZATION ITERATED SRINKAGE ALGORITHM FOR BASIS PURSUIT MINIMIZATION Michael Elad The Computer Science Department The Technion Israel Institute o technology Haia 3000, Israel * SIAM Conerence on Imaging Science

More information

Intrinsic Small-Signal Equivalent Circuit of GaAs MESFET s

Intrinsic Small-Signal Equivalent Circuit of GaAs MESFET s Intrinsic Small-Signal Equivalent Circuit o GaAs MESFET s M KAMECHE *, M FEHAM M MELIANI, N BENAHMED, S DALI * National Centre o Space Techniques, Algeria Telecom Laboratory, University o Tlemcen, Algeria

More information

Kalman filtering based probabilistic nowcasting of object oriented tracked convective storms

Kalman filtering based probabilistic nowcasting of object oriented tracked convective storms Kalman iltering based probabilistic nowcasting o object oriented traced convective storms Pea J. Rossi,3, V. Chandrasear,2, Vesa Hasu 3 Finnish Meteorological Institute, Finland, Eri Palménin Auio, pea.rossi@mi.i

More information

Virtual Array Processing for Active Radar and Sonar Sensing

Virtual Array Processing for Active Radar and Sonar Sensing SCHARF AND PEZESHKI: VIRTUAL ARRAY PROCESSING FOR ACTIVE SENSING Virtual Array Processing for Active Radar and Sonar Sensing Louis L. Scharf and Ali Pezeshki Abstract In this paper, we describe how an

More information

Vector blood velocity estimation in medical ultrasound

Vector blood velocity estimation in medical ultrasound Vector blood velocity estimation in medical ultrasound Jørgen Arendt Jensen, Fredrik Gran Ørsted DTU, Building 348, Technical University o Denmark, DK-2800 Kgs. Lyngby, Denmark Jesper Udesen, Michael Bachmann

More information

Linear Optimum Filtering: Statement

Linear Optimum Filtering: Statement Ch2: Wiener Filters Optimal filters for stationary stochastic models are reviewed and derived in this presentation. Contents: Linear optimal filtering Principle of orthogonality Minimum mean squared error

More information

Lecture Outline. Basics of Spatial Filtering Smoothing Spatial Filters. Sharpening Spatial Filters

Lecture Outline. Basics of Spatial Filtering Smoothing Spatial Filters. Sharpening Spatial Filters 1 Lecture Outline Basics o Spatial Filtering Smoothing Spatial Filters Averaging ilters Order-Statistics ilters Sharpening Spatial Filters Laplacian ilters High-boost ilters Gradient Masks Combining Spatial

More information

ANALYSIS OF A PARTIAL DECORRELATOR IN A MULTI-CELL DS/CDMA SYSTEM

ANALYSIS OF A PARTIAL DECORRELATOR IN A MULTI-CELL DS/CDMA SYSTEM ANAYSIS OF A PARTIA DECORREATOR IN A MUTI-CE DS/CDMA SYSTEM Mohammad Saquib ECE Department, SU Baton Rouge, A 70803-590 e-mail: saquib@winlab.rutgers.edu Roy Yates WINAB, Rutgers University Piscataway

More information

Objectives. By the time the student is finished with this section of the workbook, he/she should be able

Objectives. By the time the student is finished with this section of the workbook, he/she should be able FUNCTIONS Quadratic Functions......8 Absolute Value Functions.....48 Translations o Functions..57 Radical Functions...61 Eponential Functions...7 Logarithmic Functions......8 Cubic Functions......91 Piece-Wise

More information

Chem 406 Biophysical Chemistry Lecture 1 Transport Processes, Sedimentation & Diffusion

Chem 406 Biophysical Chemistry Lecture 1 Transport Processes, Sedimentation & Diffusion Chem 406 Biophysical Chemistry Lecture 1 Transport Processes, Sedimentation & Diusion I. Introduction A. There are a group o biophysical techniques that are based on transport processes. 1. Transport processes

More information

Wideband Fading Channel Capacity with Training and Partial Feedback

Wideband Fading Channel Capacity with Training and Partial Feedback Wideband Fading Channel Capacity with Training and Partial Feedback Manish Agarwal, Michael L. Honig ECE Department, Northwestern University 145 Sheridan Road, Evanston, IL 6008 USA {m-agarwal,mh}@northwestern.edu

More information

Image Enhancement (Spatial Filtering 2)

Image Enhancement (Spatial Filtering 2) Image Enhancement (Spatial Filtering ) Dr. Samir H. Abdul-Jauwad Electrical Engineering Department College o Engineering Sciences King Fahd University o Petroleum & Minerals Dhahran Saudi Arabia samara@kupm.edu.sa

More information

Parametric Signal Modeling and Linear Prediction Theory 1. Discrete-time Stochastic Processes

Parametric Signal Modeling and Linear Prediction Theory 1. Discrete-time Stochastic Processes Parametric Signal Modeling and Linear Prediction Theory 1. Discrete-time Stochastic Processes Electrical & Computer Engineering North Carolina State University Acknowledgment: ECE792-41 slides were adapted

More information

Solution to Homework 1

Solution to Homework 1 Solution to Homework 1 1. Exercise 2.4 in Tse and Viswanath. 1. a) With the given information we can comopute the Doppler shift of the first and second path f 1 fv c cos θ 1, f 2 fv c cos θ 2 as well as

More information

Virtually everything you and I know about the Cosmos has been discovered via electromagnetic

Virtually everything you and I know about the Cosmos has been discovered via electromagnetic Gravitational Waves Gravitational wave astronomy Virtually everything you and I know about the Cosmos has been discovered via electromagnetic observations. Some inormation has recently been gleaned rom

More information

Sphere Decoder for a MIMO Multi-User MC-CDMA Uplink in Time-Varying Channels

Sphere Decoder for a MIMO Multi-User MC-CDMA Uplink in Time-Varying Channels Sphere Decoder for a MIMO Multi-User MC-CDMA Uplink in Time-Varying Channels Charlotte Dumard and Thomas Zemen ftw Forschungzentrum Telekommunikation Wien Donau-City-Strasse 1/3, A-1220 Vienna, Austria

More information

Midterm Summary Fall 08. Yao Wang Polytechnic University, Brooklyn, NY 11201

Midterm Summary Fall 08. Yao Wang Polytechnic University, Brooklyn, NY 11201 Midterm Summary Fall 8 Yao Wang Polytechnic University, Brooklyn, NY 2 Components in Digital Image Processing Output are images Input Image Color Color image image processing Image Image restoration Image

More information

IEEE TRANSACTIONS ON INFORMATION THEORY, VOL. 56, NO. 1, JANUARY

IEEE TRANSACTIONS ON INFORMATION THEORY, VOL. 56, NO. 1, JANUARY IEEE TRANSACTIONS ON INFORMATION THEORY, VOL 56, NO 1, JANUARY 2010 367 Noncoherent Capacity of Underspread Fading Channels Giuseppe Durisi, Member, IEEE, Ulrich G Schuster, Member, IEEE, Helmut Bölcskei,

More information

A System for Tracking and Locating Emergency Personnel Inside Buildings

A System for Tracking and Locating Emergency Personnel Inside Buildings A System or Tracking and Locating Emergency Personnel Inside Buildings Ilir F. Progri, Student Member ION, William R. Michalson, Member ION, John Orr, and David Cyganski Electrical and Computer Engineering

More information

Root-MUSIC Time Delay Estimation Based on Propagator Method Bin Ba, Yun Long Wang, Na E Zheng & Han Ying Hu

Root-MUSIC Time Delay Estimation Based on Propagator Method Bin Ba, Yun Long Wang, Na E Zheng & Han Ying Hu International Conference on Automation, Mechanical Control and Computational Engineering (AMCCE 15) Root-MUSIC ime Delay Estimation Based on ropagator Method Bin Ba, Yun Long Wang, Na E Zheng & an Ying

More information

Q3. Derive the Wiener filter (non-causal) for a stationary process with given spectral characteristics

Q3. Derive the Wiener filter (non-causal) for a stationary process with given spectral characteristics Q3. Derive the Wiener filter (non-causal) for a stationary process with given spectral characteristics McMaster University 1 Background x(t) z(t) WF h(t) x(t) n(t) Figure 1: Signal Flow Diagram Goal: filter

More information

ANALYSIS OF SPEED-DENSITY TRAFFIC FLOW MODELS ON A MERGE INFLUENCE SECTION IN AN UNINTERRUPTED FACILITY

ANALYSIS OF SPEED-DENSITY TRAFFIC FLOW MODELS ON A MERGE INFLUENCE SECTION IN AN UNINTERRUPTED FACILITY ANALYSIS OF SPEED-DENSITY TRAFFIC FLOW MODELS ON A MERGE INFLUENCE SECTION IN AN UNINTERRUPTED FACILITY Tcheolwoong DOH Proessor Transportation Engineering University o Hanyang Sa-3dong, Sangrok-gu, Ansan

More information