Page 65 - Fundamentals of Radar Signal Processing
P. 65

(1.32)

               The  phase  correction  aligns  the  signal  component  phases  so  that  they  add
               coherently. The noise phases are still random with respect to one another. Thus,
                                                             2 2
               the integrated signal power is again N A , while the integrated noise power is
               again        ,  and  therefore  an  integration  gain  of N  is  again  achieved.
               Compensation for the phase progression so that the compensated samples add in

               phase is an example of phase history modeling: if the sample-to-sample pattern
               of target echo phases can be predicted or estimated (at least to within a constant
               overall phase), the data can be modified with a countervailing phase so that the
               full coherent integration gain is achieved. Phase history modeling is central to
               many radar signal processing functions and is essential for achieving adequate
               gains in SNR.
                     In noncoherent integration, the phases are discarded and some function of

               the magnitudes of the measured data samples are added, such as the magnitude,
               magnitude-squared, or log-magnitude. If the magnitude-squared is chosen, then z
               is formed as


















                                                                                                       (1.33)

               The important fact is that phase information in the received signal samples is
               discarded.
                     The first line of Eq. (1.33) defines noncoherent square-law integration. The
               next two lines show that, because of the nonlinear magnitude-squared operation,
               z cannot be expressed as the sum of a signal-only part and a noise-only part due

               to the presence of the third term involving cross-products between signal and
               noise components. A similar situation exists if the magnitude or log-magnitude
               is  chosen  for  the  noncoherent  integration.  Consequently,  a  noncoherent
               integration gain cannot be simply defined as it was for the coherent case.
                     It  is  possible  to  define  a  noncoherent  gain  implicitly.  For  example,  in
               Chap. 6 it will be seen that detection of a constant-amplitude target signal in
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