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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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784 CHAPTER 17 Advanced Processing Methods for Passive Bistatic <strong>Radar</strong> SystemsAs previously mentioned, in FUSC mode the variable pilots position is different for evenandodd-numbered OFDM symbols. However, frequency spacing among variable pilotswithin an OFDM symbol is constant and equal to 12f. Considering the alternate transmissions<strong>of</strong> odd and even symbols and the relative displacement <strong>of</strong> the pilots subcarrierssets between consecutive symbols, the whole set A V <strong>of</strong> intrasymbol side peaks due tovariable pilots can be written asA V ={(n T U6 , i ); n ∈T S{((2n + 1) T U12 , 2i + 1 ); n ∈2T S[ ⌊1, ..., 6 T ⌋ ] }S− 1 ; i ∈ Z ∪T U[ ⌊1, ..., 6 T ⌋ ] }S− 1 ; i ∈ ZT U(17.32)Notice that the temporal separation, T U /6, between peaks corresponds to the inverse <strong>of</strong>the frequency displacement, 6f, between the pilots subcarriers sets exploited by odd andeven symbols. In Figure 17-21b, the first five intrasymbol side peaks due to variable pilotsare labeled with stars.Similarly the set B V <strong>of</strong> intersymbol side peaks caused by variable pilots is given byB V = {(2qT S , 0) ; q ∈ N} ∪{(qT S + T G + n T U6 , i )T S; n ∈{(qT S + T G + (2n + 1) T U12 , 2i + 1 ); n ∈2T S[ ⌊1, ..., 6 T ⌋ ]}S− 1 ; q ∈ N; i ∈ Z ∪T U[ ⌊1, ..., 6 T ⌋ ]}S− 1 ; q ∈ N; i ∈ ZT U(17.33)In Figure 17-21b, the first six intersymbol side peaks due to variable pilots are labeled withsquares. As expected, the first peak <strong>of</strong> this set appears at τ = T S + T G + T U /6 = 126.9 μs(T G = T U /8 in the considered example). Notice that the level <strong>of</strong> side peaks due to variablepilots is greater than the level <strong>of</strong> side peaks due to fixed pilots since a higher number <strong>of</strong>subcarriers is devoted to variable pilots.Obviously, side peak distributions are different for FUSC and PUSC transmissionmodes [15]. However, the obtained PSLR is comparable in the two cases. Specifically, thePSLR is dominated by the peak caused by the guard interval whose level has a theoreticalvalue equal to 20log 10 (T G /T U ) = –18 dB with respect to the main peak.Regarding the distribution <strong>of</strong> side peaks in the Doppler dimension, the first Dopplerside peak set (due to the preamble subcarriers allocation) appears at a Doppler frequencycorresponding to the inverse <strong>of</strong> the temporal separation between consecutive DL frames(1/T frame ). However, the preamble contribution to the AF <strong>of</strong> the whole DL frame canbe reasonably neglected. In any case, the single OFDM symbol corresponding to thepreamble might be left out <strong>of</strong> the integration time with a very small SNR degradation.Consequently, the first Doppler side peak set due to pilot tones appears at a Dopplerfrequency equal to f D = 1/2T S = 4.96 kHz. This Doppler frequency value correspondsto a bistatic velocity <strong>of</strong> about 765 km/h (in the worst case a 3.5 GHz carrier frequency).However, additional sidelobe structures appear at a Doppler frequency equal to 500 Hz(Figure 17-21). Such peaks are obviously because <strong>of</strong> the pulsed nature <strong>of</strong> the consideredsignals that consist <strong>of</strong> DL frames <strong>of</strong> duration T DL transmitted every T frame . The Dopplerambiguities result from the equivalent PRF = 1/T frame , which is not within the control <strong>of</strong>the radar designer. As an example, for the 2 ms frame duration considered in Figure 17-21,

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