Page 513 - Fundamentals of Radar Signal Processing
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multiplier α. Approximately the same relationship will determine the detection

               probability   attained with the new threshold multiplier α′ and SNR  .  will
               equal   if






                                                                                                     (6.150)

               Using Eq. (6.148) in Eq. (6.150) leads to






                                                                                                     (6.151)

               Figure 6.23b plots the approximate “target masking loss”                  in decibels for the
               same conditions as in Fig. 6.23a.

                     The results given in Eqs. (6.149) and (6.151) are only approximations. A
               more careful analysis would mimic the basic CA CFAR analysis of Sec. 6.5.3
               by finding the PDF of the threshold in the presence of an interfering target, then
               using  that  PDF  to  find  the  expected  values  of P   and P .  This  approach  is
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               complicated by the fact that the interfering target changes the PDF of the cell
               containing  it.  For  instance,  if  the  interferer  is  nonfluctuating  the  PDF  of  the
               power in its cell will be a generalized noncentral chi-squared, while all of the
               remaining cells will still be exponentially distributed. The PDF of the threshold

               will be a mixture of the noncentral chi-squared and exponential PDFs. To avoid
               calculating  this  PDF,  the  expected  value  of  the  threshold  was  used  in  the
               expressions  for  the  case  of  no  interfering  target.  This  gives  a  simple
               approximation  that  behaves  correctly  in  the  limits  of  large  and  small  mean
               interferer SNR  .

                     Figure 6.24 illustrates a related phenomenon, self-masking by a distributed
               target. The interference, detector, and target characteristics are the same as in
               Fig. 6.20, with the exception that the physical extent of the target is now greater
               than  a  range  bin  so  that  the  target  signature  is  spread  over  three  consecutive
               cells. Figure 6.24a shows the effect when no guard cells are used. When one of
               the three target cells is the test cell, the other two contaminate the interference
               estimate, raising the threshold just enough to prevent detection. This effect is the

               reason  for  using  guard  cells.  Their  impact  is  illustrated  in Fig. 6.24b, where
               three guard cells are used to each side of the test cell. This lengthens the total
               CFAR window slightly, but assures that when the test cell is centered on the
               target, the adjoining target cells do not contaminate the interference estimate and
               the target is now detected.
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