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of the autocorrelation function of the clutter and the MTI filter impulse response

               (Levanon, 1988; Nathanson, 1991). For low-order filters such as two- or three-
               pulse cancellers and clutter power spectra with either measured or analytically
               derivable  autocorrelation  functions,  the  resulting  equations  can  be  easier  to
               evaluate than the frequency domain versions.
                     As an example of the autocorrelation approach, consider the output of the
               two-pulse canceller when the input is just clutter; this is c′[m] = c[m]  – c[m –

               1]. The expected value of the filter output power is




                                                                                                       (5.52)

                                                                                6
               where  Re{·}  denotes  the  real  part  of  the  argument.   Assuming  that c[m]  is
               stationary,




                                                                                                       (5.53)

               where




                                                                                                       (5.54)

               is  the  autocorrelation  function  of c[m].  Note  that                  . Also  define  the
               normalized autocorrelation function






                                                                                                       (5.55)

               The clutter attenuation component of the improvement factor in Eq. (5.48) can
               now be written as












                                                                                                       (5.56)

               As  noted  above,  the  gain  for  a  two-pulse  canceller  is G  =  2;  thus  the
               improvement factor for the two-pulse canceller is
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