Tài liệu Adaptive WCDMA (P3) pdf

3 Code acquisition 3.1 OPTIMUM SOLUTION In this case, the theory starts with a simple problem where, for a received signal r(t) = s(t, θ) + n(t), we have to estimate a generalized time invariant vector of parameters θ (frequency, phase, delay, data, .) of a signal s(t, θ) in the presence of Gaussian noise n(t). The best that we can do is to find an estimate ˆ θ of the parameter θ for which the aposterior probability p( ˆ θ/r) is maximum; hence the name maximum aposterior probability (MAP) estimate. In other words, the chosen estimate based on the received signal r is correct for the highest probability. Practical implementation requires us to locally generate a number of trial values ˜ θ,toevaluatep( ˜ θ/r) for each such value and then to choose ˜ θ = ˆ θ for which p( ˜ θ/r) is maximum. In this chapter, we focus only on code acquisition and parameter θ will include only code delay θ ={τ } and become a scalar. Analytically, this can be expressed as MAP ⇒ ˆ θ = arg max p( ˜ θ/r) (3.1) Very often, in practice, evaluation of p( ˜ θ/r) in closed form is not possible. By using the Bayesian rule for the joint probability distribution function p(r, ˜ θ) = p(r)p( ˜ θ/r) = p( ˜ θ)p(r/ ˜ θ) (3.2) and assuming a uniform prior distribution of θ, maximizing p( ˜ θ/r) becomes equivalent to maximizing p(r/ ˜ θ), a function that can be determined more easily. This algorithm is known as maximum likelihood (ML) estimation and can be defined analytically as ML ⇒ ˆ θ = arg max p(r/ ˜ θ) (3.3) It is straightforward to show that in the case of Gaussian noise, the ML principle necessi- tates the search for that value of θ that would maximize the likelihood function defined as λ( ˜ θ) =  r(t)s(t, ˜ θ)dt −  s 2 (t, ˜ θ)dt(3.4) Adaptive WCDMA: Theory And Practice. Savo G. Glisic Copyright ¶ 2003 John Wiley & Sons, Ltd. ISBN: 0-470-84825-1 44 CODE ACQUISITION where s(t, ˜ θ) is the locally generated replica of the signal with a trial value ˜ θ.For the given signal power, the second term in the previous equation is a constant so that the maximization is equivalent to the maximization of the first term only. This can be expressed as λ( ˜ θ) =  r(t)s(t, ˜ θ)dt(3.5) Instead of searching for the maximum of λ( ˜ θ) in a so-called open loop configuration, an equivalent procedure would be to find the zero of the first derivative of λ( ˜ θ) MLT ⇒ ˆ θ = arg zero ∂λ( ˜ θ) ∂ ˜ θ = arg zero  r(t) ∂s(t, ˜ θ) ∂ ˜ θ dt (3.6) This structure is known as the maximum likelihood tracker (MLT). In practice, the signal derivative is often approximated by the signal difference ∂s(t, ˜ θ) ∂ ˜ θ = 1 2θ {s(t, ˜ θ + θ ) − s(t, ˜ θ − θ)} (3.7) where s(t, ˜ θ + θ ) and s(t, ˜ θ − θ ) are so called early and late versions of the local signal with respect to the generalized parameter θ to be estimated. This results in the so-called early–late tracker ELT ⇒ ˆ θ = arg zero{E(t, ˜ θ) − L(t, ˜ θ)} (3.8) where E(t, ˜ θ) = 1 2θ  r(t)s(t, ˜ θ + θ )dt L(t, ˜ θ) = 1 2θ  r(t)s(t, ˜ θ − θ )dt (3.9) In the case of code synchronization, θ = τ and the ML synchronizing receiver implied by equation (3.5) should, in principle, create all possible time-offset versions of the known code waveform, correlate all of them with the received data and choose the ˜τ corre- sponding to the largest correlation as its estimate, ˆτ ML . Owing to the continuous range of values of τ , this is not possible in practice and some type of range quantization is necessary. The resulting candidate values are called cells, and the initial parameter esti- mation problem is translated into a multiple-hypothesis problem: to locate the cell most likely to contain the unknown offset, given this piece of data. This is exactly the coarse code synchronization or code acquisition problem, the result of which is to resolve the code phase (or the ‘epoch’) ambiguity within the size of the cell. Since this remaining error is typically larger than desired, further operations are required in order to reduce it to acceptable levels. This remaining part of the synchronization task, namely, that of PRACTICAL SOLUTIONS 45 fine synchronization or code tracking, is performed by one of the available code-tracking loops, which we discuss in the next chapter. Once the nature and size of these cells have been determined, the next question is how to go about performing the search most successfully. Clearly, the strategy will depend on a variety of factors such as criteria of performance, degree of complexity and computational power available (directly related to cost), prior available information about the location of the correct cell and so on. A brute-force approach would try to create a bank of parallel correlation branches, each matched to a possible quantized value of the timing offset; it would then process the received waveform through all of them simultaneously, pick the largest and declare a candidate solution. Unless the uncertainty region (number of cells) is small, corresponding to either a small code period or a small initial uncertainty, such a solution (which we may call the totally parallel solution) becomes obviously unwieldy in complexity very quickly. We note, however, that small uncertainty regions may be encountered in a nested design, whereby a multitude of different-period codes are combined for precisely the purpose of aiding acquisition. Furthermore, neural network structures are currently being explored for this purpose, where the neural network is trained for all possible such values. Such a scheme would emulate the spirit (if not the exact statistical processing) of the above solutions. 3.2 PRACTICAL SOLUTIONS In practice, most of the time total parallelism is out of the question when the number of cells is very large (although it appears doable for smaller uncertainty regions) and simpler solutions are necessary. One of the most familiar of such approaches is the simple technique of serial search, where the search starts from a specific cell and serially examines the remaining cells in some direction and in a prespecified order until the correct cell is found. Hence, serial search techniques do not account for any additional information gathered during the past search time, which could conceivably be used to alter the direction of search toward cells that show increased posterior likelihood of being the correct ones. A serial search starts from a cell that could be chosen totally arbitrarily (no prior information), or by some prior knowledge about a likely cell, and proceeds in a simple and easily implementable predirected manner. When the uncertainty space (collection of all possible cells) is two-dimensional (delay and frequency offset) and searching all possible cells serially appears to be very time consuming, a speedup may be achieved by employing a bank of filters, each matched to a possible Doppler offset. The same idea can be applied to the one-dimensional case (no frequency uncertainty), where now a bank of correlators may be employed, each starting from a different point of the uncertainty region. This effectively amounts to dividing the search in many parallel subsearches and therefore reducing the total search time by a proportional amount. One should be aware that although it holds true that only one cell contains the exact delay and Doppler offsets of the incoming code, the set of desirable cells acceptable to the receiver includes a number of cells adjacent to the exact one. Indeed, the receiver will terminate acquisition and initiate tracking, the first time a cell is reached (and correctly identified), which is close enough to true synchronization so that the tracking loop can pull 46 CODE ACQUISITION in and perform the remaining synchronization operation successfully. All these desirable cells are collectively called hypothesis H 1 , and the remaining nondesirable ‘out-of-sync’ cells comprise hypothesis H 0 . As an example, consider the case in which the receiver examines the code delay uncertainty in steps of half a chip time (δt = T c /2) and there is no frequency uncertainty. Then, all four cells located in the interval (−T c ,T c ) around the true delay of the incoming code are included in hypothesis H 1 , since some amount of code correlation exists for each one of these cells, an amount that can initiate the code-tracking loop. The above definition of cells and hypotheses implies that each test does not pertain to a single value of the unknown parameter τ , but rather to a range of values. It is straightforward to show that, under mild conditions and approximations pertaining to the pseudorandom nature of the code, this reformulated hypothesis testing results in a statistic (correlation) and threshold setting that do not depend on the given (tested) value of the unknown parameter (a uniformly most powerful test). This is because the threshold value is set by the desirable probability of false alarm per cell (see below), which is independent of τ under H 0 . To recapitulate, the two-dimensional time/frequency code offset uncertainty within the noisy received waveform is quantized into a number of cells, which are typically searched in a serial fashion by a correlation receiver, although parallel multiple branches are also possible. Motivated by an ML argument, the receiver creates a cross-correlation between the incoming waveform and the local code at a specific offset, whose output is used to decide whether the currently examined cell is a desirable (H 1 ) one. The process continues until one such cell is correctly identified. At that point, acquisition is terminated and tracking is initiated. 3.3 CODE ACQUISITION ANALYSIS The serial code acquisition can be represented by using the signal flow graph theory. Each cell is represented by a node of a graph and transitions between the nodes depend on the outcome of the decision in a given cell. Branches connecting the nodes characterize these transitions. To motivate the operation in a transform domain, let us consider the simple model of a process represented by the graph in Figure 3.1 and evaluate the probability p ac (t) that the process will move from a to c in exactly t seconds. To do this, we will introduce an additional variable τ to designate the time needed for the process to move from a to b, characterized by the probability p ab (τ ). The parameter a b c t t Figure 3.1 Signal flow graph for a 3-state process. CODE ACQUISITION ANALYSIS 47 p ac (t, τ ) represents the joint probability that the process moves from a to c in t seconds and takes τ seconds to move from a to b. This probability can be represented as p ac (t, τ ) = p ab (τ )p bc (t − τ) (3.10) resulting in p ac (t) =  p ac (t, τ ) dτ =  p ab (τ )p bc (t − τ)dτ = p ac (t) ∗ p bc (t) (3.11) In other words, the overall probability p ac (t) is a convolution of the two intermode transition probabilities p ab and p bc . It is clear that for the graph with a large number of nodes we will have to deal with multiple convolutions giving rise to computational complexity. In this case, people being involved in electrical engineering prefer to move to a transform domain, either Laplace (s) domain for continuous variables or into z-domain for desecrate variables. This leads to using z-transform for the decision process flow graph representation and multiple convolutions will be now replaced with multiple products making the calculus much simpler. If p ij (n) is the probability for the process to move from node i to node j in exactly n steps, then its z-transform P i,j (z) = ∞  n=0 z n p ij (n) (3.12) is called the probability generating function. For the analysis to follow, we will need a few relations derived from this definition. First of all, the first and the second derivative of this function can be represented as ∂ ∂z P ij (z) = ∞  n=0 np ij (n)z n−1 (3.13) ∂ 2 ∂z 2 P ij (z) = ∞  n=0 n(n − 1)p ij (n)z n−2 (3.14) By definition, the average number of steps to move from node i to node j is n = ∞  n=0 np ij (n) = ∂ ∂z P ij (z)     z=1 (3.15) and the average time to do it can be represented as t ij = T ij = nT =  ∂ ∂z P ij (z)     z=1  · T(3.16) 48 CODE ACQUISITION where T is the cell observation time that is, the time needed to create the decision variable that will be referred to as dwell time. For the variance, we start with the definition σ 2 T = (n 2 − n 2 )T 2 (3.17) The second derivative of the generating function can be represented as ∂ 2 ∂z 2 P ij (z)     z=1 = ∞  n=0 n 2 p ij (n) − ∞  n=0 np ij (n) = n 2 − n(3.18) By using equations (3.15) and (3.18) in equation (3.17), the variance of time t ij can be expressed in the following form: σ 2 T =  ∂ 2 P ij (z) ∂z 2 + ∂P ij (z) ∂z −  ∂P ij (z) ∂z  2  z=1 T 2 (3.19) In what follows, we will use these few relations to analyze serial search code acquisition. In order to get an initial insight into this method, we will assume that there are q cells to be searched. Parameter q may be equal to the length of the pseudonoise (PN) code to be searched or some multiple of it. For example, if the update size is one-half chip, q will be twice the code length to be searched. Further assume that if a ‘hit’ (output is above threshold) is detected by the threshold detector, the system goes into a verification mode that may include both, an extended duration dwell time and an entry into a code loop tracking mode. In any event, we model the ‘penalty’ of obtaining a false alarm as Kτ d second and the dwell time itself as τ d second. If a true hit is observed, the system has acquired the signal, and the search is completed. Assume that the false alarm probability P FA and the probability of detection P D are given. We will also assume that only one cell represents the synchro position. Let each cell be numbered from left to right so that the kth cell has apriori probability of having the signal present, given that it was not present in cells 1 through k − 1, of p k = 1 q + 1 − k (3.20) The generating function flow diagram is given in Figure 3.2 using the rule that at each node the sum of the probability emanating from the node equals unity. The unit time rep- resents τ d seconds and Kτ d seconds are represented in z-transform by z K . Consider node 1. The apriori probability of having the signal present is P 1 = 1/q, and the probability of it not being present in the cell is 1 − P 1 . Suppose the signal was not present. Then we advance to the next node (node 1a); since it corresponds to a probabilistic decision and not a unit time delay, no z multiplies the branch going to it. At node 1a a false alarm may occur, with probability P FA = α. This would require one unit of time to decide (τ d s) and then K units of time (Kτ d s) are needed in verification mode to determine that there was a false alarm. False alarms will not occur with probability (1 − α). This would take one dwell time to decide and is represented by (1 − α)z branch going to node 2. CODE ACQUISITION ANALYSIS 49 F S P D Z P 1 P FA3 Z k +1 P FA1 Z k +1 P FAq Z k +1 P FA2 Z k +1 (1− P FAq )Z (1− P FA1 )Z (1− P D )Z 1− P 1 (1− P FA3 )Z (1− P FA2 )Z 1 1 1 1 2 3 4 F P D Z P 2 P FA4 Z k +1 P FA2 Z k +1 P FA1 Z k +1 P FA3 Z k +1 (1− P FA1 )Z (1− P FA2 )Z (1− P D )Z 1− P 2 (1− P FA4 )Z (1− P FA3 )Z 2 2 2 3 3 4 5 F P D Z P 4 P FA2 Z k +1 P FAq −1 Z k +1 P FAq −1Z k +1 P FA1 Z k+1 (1− P FAq −1)Z (1− P FA −1 )Z (1− P D )Z q −1 q −1 (1− P FA2 )Z (1− P FA1 )Z 1 1 3 2 1 12 q Deterministic model of the acquisition time: Flow graph of the generating function * q -valued P FA i ( P FA i , i = 1, 2, , q ) *Constant P D Figure 3.2 Code acquisition decision process flow graph. 50 CODE ACQUISITION Now consider the situation at node 1 when the signal is present. If a hit occurs (that is, the signal is detected), then acquisition, as we have defined it, occurs and the process is terminated in node F denoting ‘finish’. If there was no hit at node 1 (the integrator output was below the threshold), which occurs with probability 1 − P D , one unit of time would be consumed for such a decision. This is represented by the branch (1 − P D )z leading to node 2. At node 2, in the upper left part of the diagram, either a false alarm occurs with probability α and delay (K + 1), or a false alarm does not occur with a delay of 1 unit. The remaining portion of the generating function flow graph is a repetition of the portion just discussed with the appropriate node changes. At this stage we will assume that only Gaussian noise is present so that P FA and P D are the same for each cell. By using standard signal flow graph reduction techniques [1], one can show that the overall transfer function between nodes S (start) and F (finish) can be represented as U(z) = (1 − β) 1 − βzH q−1 1 q   q−1  l=0 H l (z)   (3.21) where H(z) = αz K+1 + (1 − α)z and β = 1 − P D (3.22) By using equation (3.16), the mean acquisition time is given (after some algebra [1]) by T = 2 + (2 − P D )(q − 1)(1 + KP FA ) 2P D τ d (3.23) with τ d being included in the formula to translate from our unit timescale. For the usual case, when q  1, the mean acquisition time T is given by T = (2 − P D )(1 + KP FA ) 2P D (qτ D )(3.24) The variance of the acquisition time is given by equation (3.19). It can be shown that the expression for σ 2 is σ 2 = τ 2 d  (1 + KP FA ) 2 q 2  1 12 − 1 P D + 1 P 2 D  + 6q[K(K + 1)P FA (2P D − P 2 D ) (3.25) + (1 + P FA K)(4 − 2P D − P 2 D )] + 1 − P D P 2 D  In addition, when K(1 + KP FA )  q,then σ 2 = τ 2 D (1 + KP FA ) 2 q 2  1 12 − 1 P D + 1 P 2 D  (3.26) CODE ACQUISITION IN CDMA NETWORK 51 As a partial check on the variance result, let P FA → 0andP D → 1. Then we have σ 2 = (qτ D ) 2 12 (3.27) which is the variance of a uniformly distributed random variable, as one would expect for the limiting case. The above results provide a useful theoretical estimate of acquisition time for an idealized PN-type system. In practice, two basic modifications should be made to make the estimates reflect actual hardware or software systems. First, Doppler effects should be taken into account. The result of code Doppler is to smear the relative code phase during the acquisition dwell time, which increases or reduces the probability of detection depending on the code phase and the algebraic sign of the code Doppler rate. The Doppler also affects the effective code sweep rate, which in the extreme case can reduce it to zero to cause the search time to increase greatly. This topic will be discussed later. The second refinement to the model concerns the handover process between acquisition and tracking. Typically after a ‘hit’ the code-tracking loop is turned on to attempt to pull the code into tight lock. Further, often in low signal-to-noise ratio (SNR) systems in which both acquisition (pull-in) bandwidth and tracking bandwidth are used, multiple code loop bandwidths will be employed in order to soften the transition between acquisition and tracking modes. Consequently, the probability of going from the acquisition mode to the final code loop bandwidth in the tracking mode occurs with some probability less than 1. The estimation of this probability is at best a very difficult problem (although, some approximate results have been developed). At high SNRs, this probability quickly approaches 1, so it is not a problem. At low SNRs, the above formula for acquisition time should replace P D with P  D P  D = P D P HO (3.28) with P HO being the probability of handover. In the S-band shuttle system, at TRW it was found that at threshold (C/N 0 = 51 dB Hz) P HO varied from 0.06 to 0.5 depending upon the code Doppler. Without code Doppler P HO was 0.25, which, if not taken into account in the acquisition time equation, would predict the mean acquisition time to be about four times too fast. 3.4 CODE ACQUISITION IN CDMA NETWORK The previous Section 3.3 is limited to the case of spread-spectrum signal in Gaussian channel. In that case, the probability of false alarm in all nonsynchro cells is the same. In a communication radio network, the interfering signal is the sum of Gaussian noise and overall multiple access interference (MAI). In each cell, i, MAI has a different value so that P FAi = P FAj for each i = j . In such a case, under the assumption of a static channel, the serial acquisition process can be modeled again by the graph from Figure 3.2 with P FA being different for each cell. We will first deal with a simpler problem in which the proba- bility of signal detection P D does not depend on MAI. Besides being simpler, this model is still valid for an important class of these systems called quasi-synchronous Code Division 52 CODE ACQUISITION Multiple Access (CDMA) networks. In these networks, all users are synchronized within the range between zero delay and the position of the first significant cross-correlation peak. Examples of such systems are described for both satellite and land mobile CDMA communication systems. The average acquisition time is obtained by using the same steps as in the previ- ous section. The details are presented in Reference [2]. The result, after a cumbersome manipulation of very long equations can be expressed as T acq = [2 + (q − 1)(1 + kP FA )(2 − αP D )] τ d 2P D (3.29) where α = 1 + kρ 1 + kP FA (3.30) with ρ = 2 q(q − 1)  q  i=1 (i − 1)P FAi  (3.31) and P FA = 1 q q  i=1 P FAi (3.32) By inspection, we can see from equation (3.29) that the minimum average acquisition time is obtained for large values of parameter α. Besides P FA , this parameter also depends on the position of the cells with high P FAi within the code delay uncertainty region. The set of P FAi , representing the probability distribution function of P FA , will be called MAI pattern or MAI profile. From equation (3.31), one can see that for a large α , the products iP FAi should be large. This means larger P FAi for larger i. That means that hopefully, synchronization will be acquired before we get to the region with high P FA or in the case of multiple sweep of the uncertainty region, we will have smaller numbers of sweeps of the region. In an asynchronous network, MAI takes on different values in all cells including the synchro cell so that, in general, P D is different. In such a case, the average acquisition time becomes [2] T acq = τ d 2 ˜ P D [2 + (1 + kP FA )(q − 1)(2 − α ˜ P D ) + 2k(P FA − P R ˜ P D )] (3.33) where P FA = 1 q q  i=1 P FAi , P R = 1 q q  i=1 P FAi P Di , ˜ P D =  1 q q  i=1 1 P Di  −1 α = 1 + kρ 1 + kP FA and ρ = 2 q(q − 1)  q  i=1 (i − 1)P FAi  (3.34) [...]... interference) Adaptive threshold setting (nonuniform interference) Adaptive integration time (nonuniform interference) Up-ranked cells algorithm (nonuniform interference) 3500 3000 2500 2000 × × 1500 × × × × 5 6 7 1000 1 2 3 4 × 8 × 9 10 No of angular cells used for acquisition (m) Figure 3.18 Performance comparison of two-dimensional code acquisition (FASD search) with adaptive integration time and adaptive. .. interference) Adaptive threshold setting (nonuniform interference) Adaptive integration time (nonuniform interference) Up-ranked cells algorithm (nonuniform interference) 3500 3000 × 2500 2000 × × × 1500 × × × × 7 8 × 1000 1 2 3 4 5 6 9 10 No of angular cells used for acquisition (m) Figure 3.19 Performance comparison of two-dimensional code acquisition (FASD search) with adaptive integration time and adaptive. .. the performance tends to approach the performance of the equivalent uniformly distributed interference case Similar improvements can be achieved by using adaptive integration time or threshold setting keeping CFAR The mean acquisition time for the adaptive integration time approach is obtained after some cumbersome algebraic manipulation of the generating function, resulting in Reference [7] Tma = 1... Zoltowski, M and Liu, H (2000) Low-complexity space-time processor for DSCDMA communications IEEE Trans Signal Process., 48(1), 39–52 35 Wang, B and Kwon, H M (2000) PN code acquisition with adaptive antenna array and adaptive threshold for DS-CDMA wireless communications Proc IEEE GLOBECOM , San Francisco, CA, pp 152–156 36 Wang, B and Kwon, H M (2000) PN code acquisition using smart antenna for DS-CDMA... spread spectrum signals in multipath channels using antenna arrays Proc MILCOM ’95 Conference, Vol 3, November 1995, pp 1170–1174 22 Dlugos, D and Scholtz, R (1989) Acquisition of spread spectrum by an adaptive array IEEE Trans Acoustics, Speech Signal Process., 37(8), 1253–1270 23 Hopkins, P M (1977) A unified analysis of pseudonoise synchronization by envelope correlation IEEE Trans Commun., 25, 770–778... integration time, in the original environment (nonuniform interference distribution, FASD search) and in an equivalent uniform distribution of the same power is used as reference The improvements obtained by adaptive schemes are evident 3.8 CELL SEARCH IN W-CDMA In this section, we discuss specific solutions for cell search in the UMTS system The cell search itself is divided into five acquisition stages: slot . function defined as λ( ˜ θ) =  r(t)s(t, ˜ θ)dt −  s 2 (t, ˜ θ)dt(3.4) Adaptive WCDMA: Theory And Practice. Savo G. Glisic Copyright ¶ 2003 John Wiley