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(4.118)

               where K is the window length. The loss in SNR at the matched filter output is
               called the processing loss (PL) and is









                                                                                                     (4.119)

               With these definitions LPG and PL are both greater than one so that the losses in
               decibels are positive numbers. For a relatively long Hamming window, the LPG
               is approximately 5.4 dB while the PL is approximately 1.4 dB. Both are weak
               functions  of K  and  are  slightly  larger  for  small K.  These  formulas  are
               approximate when applied to windowing of the LFM spectrum due to the finite-
               width transition of the LFM spectrum and the designer’s discretion in choosing

               the cutoff of the window in frequency. In the example above, the LPG is 5.35
               dB. Derivation of these formulas is deferred to Chap. 5, where they will arise
               again in the context of Doppler processing and where the results will be exact.


               4.7.2   Matched Filter Impulse Response Shaping
               The  impulse  response  of  the  filter  just  obtained  and  illustrated  in Fig.  4.34b
               suggests that similar results could have been obtained by windowing the LFM
               waveform in the time domain. Consider again the signal in Eq. (4.89) having an

               arbitrary  amplitude  function A(t)  and  a  quadratic  phase  function.  The  PSP
               approximation  to  its  spectrum  was  given  in Eq. (4.93). The magnitude of the
               spectrum is proportional to the time-domain amplitude:






                                                                                                     (4.120)

               If A(t) has finite support on –τ/2 ≤ t ≤ τ/2, it follows that X(Ω) will have finite
               support  on –β/2  ≤ F  ≤ β/2 and in that interval|X(Ω)|has the same shape as the

               window magnitude | A(t)|. Thus, a Hamming-shaped (for example) spectrum can
               be  obtained  by  applying  a  Hamming  window  to  the  impulse  response h(t)
               instead of the frequency response H(F). Note that this result is specific to the
               use of a linear FM waveform.
                     The output of the resulting filter is overlaid on the matched filter response
               i n Fig.  4.36.  It  has  the  same  general  character  as  the  frequency-domain
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