Page 506 - Fundamentals of Radar Signal Processing
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target  is  in  the  lagging  reference  window.  When  a  target  is  in  the  reference

               window,  the  assumption  that  all  of  the  reference  cells  share  the  same
               interference  statistics  as  the  test  cell  is  violated  and  the  estimate  of  the
               interference power is unreliable. However, when the test cell is located at the
               cell containing the target, the reference windows contain only noise samples and
               the threshold falls to an appropriate level, allowing target detection. The extent
               of the elevated threshold regions to either side of a target equals the extent of the

               leading and lagging windows. The extent of the region of normal threshold level
               between the two elevated regions equals the total number of guard cells plus
               one (for the test cell).

                     As the number of reference cells N becomes large, the estimate                   should

               converge  to  the  true  value        and the average probabilities of detection and
               false alarm should also converge to the values obtained in Sec. 6.3.4. To see
               this, it is easier to work with ln   than with   itself:












                                                                                                     (6.138)

               Taking the limit as N → ∞






                                                                                                     (6.139)

               Similarly





                                                                                                     (6.140)

               Combining Eqs. (6.139) and (6.140) gives the relation:





                                                                                                     (6.141)

               which  is  identical  to Eq.  (6.101)  for  a  Swerling  1  target,  no  noncoherent
               integration, and a known interference power.
                     All of the previous discussion has been for a square-law detector. Similar
               analyses  can  be  carried  out  for  a  linear  detector,  but  the  results  are  more
               difficult to obtain in closed form. Suppose that the measurements {w} are the
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