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Principles of Modern Radar - Volume 2 1891121537

Principles of Modern Radar - Volume 2 1891121537

Principles of Modern Radar - Volume 2 1891121537

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754 CHAPTER 17 Advanced Processing Methods for Passive Bistatic <strong>Radar</strong> Systemsfurther approximation <strong>of</strong> the batches algorithm described already. To show its derivation,we first rewrite equation (17.2) and then replace the cross-correlation between the r-thportions <strong>of</strong> length n C <strong>of</strong> the surveillance and the reference signals, with its approximationevaluated in the frequency domain:χ[l,m] ∼ =∼=N∑C −1r=0N∑C −1r=0= 1mr− j2πen∑C −1N Cp=0mr− j2π 1Ne Cn∑C −1kl+ j2πen Ck=0s surv [rn C + p] · s ∗ ref [rn C + p − l]n∑C −1S (r)n Ck=0N∑C −1n Cr=0surv [k]S(r)∗ refkl+ j2πn[k]e Cmr− j2πNY [k,r]e C (17.10)Notice that by neglecting the border effects (additional approximation with respect tothe batches algorithm), the r-th subsequences are cyclically extended so that their crosscorrelationcan be evaluated in the frequency domain, as the IDFT <strong>of</strong> their individual DFTs[k] and S(r)∗[k] in the second line). By rearranging the terms <strong>of</strong> the summations, the(S (r)survrefthird line <strong>of</strong> equation (17.10) is easily obtained.The resulting algorithm (sketched in Figure 17-4b) can be subdivided into four steps:1. Evaluate the DFTs <strong>of</strong> surveillance and reference signals over the N C batches <strong>of</strong> n Csamples each.2. Compute the product <strong>of</strong> the DFTs outputs for each batch and arrange the results in the2-D sequence Y [k,r] = Ssurv (r) [k]S(r)∗ ref [k](k = 0,...,n C − 1; r = 0,...,N C − 1).3. Evaluate the DFT X[k,m] <strong>of</strong>Y [k,r] over the index r for each k (n C IDFTs); this steprepresents the parallel processing <strong>of</strong> the n C different frequency channels in which thesignals have been split.4. Evaluate the IDFT <strong>of</strong> X[k,m] over the index k for each m (N C DFTs) to obtain therange samples <strong>of</strong> the 2D-CCF at the m-th Doppler bin.Notice that evaluating the DFT <strong>of</strong> short subsequences (Step 1) separates each sequenceinto a number <strong>of</strong> frequency channels (channelization) that are independently processed(Steps 2 and 3) and then recombined to provide the final result (Step 4).The computational load for the channelization technique is reported in Table 17-1 asa function <strong>of</strong> the number n C <strong>of</strong> channels assuming n C N C = N. In this case, the number<strong>of</strong> frequency channels is equal to the batches length; thus, the algorithm parameters mustbe selected so that N C ≥ N f . Moreover, since the range samples <strong>of</strong> the 2D-CCF areobtained from the last DFT stage performed over sequences <strong>of</strong> n C samples, assuming thatonly positive values <strong>of</strong> the differential bistatic range R B are included in the 2D-CCF map,n C ≥ 2N τ should be satisfied. Reducing n C within these limits allows a correspondingreduction in the computational load.The number <strong>of</strong> channels should be carefully selected since it yields a trade-<strong>of</strong>f betweenthe two adopted approximations <strong>of</strong> equation (17.10) that determine the final SNR loss.Increasing n C yields a higher integration loss for fast-moving targets whose Doppler shiftis not properly compensated (as for the batches algorithm) [28]. However, in this case,reducing n C enhances the border effects in the evaluation <strong>of</strong> the batches cross-correlationsyielding additional loss for targets at higher bistatic ranges. Assuming a constant modulus

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