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FIGURE 4.56   Autocorrelation of an N = 51 polyphase Barker code.











               The  PSL  is  –34.2  dB,  significantly  better  than  the  –24.6  dB  for  the  51-point
               MPS code in Table 4.2.


               4.10.3   Mismatched Phase Code Filters

               The sidelobe structure of phase-coded waveforms can be improved with the use
               o f mismatched  filters,  just  as  is  done  with  stepped  frequency  and  FM
               waveforms to improve their sidelobe structures. For phase-coded waveforms,
               this implies correlating the code sequence with another discrete-time sequence,
               not necessarily restricted in the amplitudes or phases of its coefficients, such
               that some metric of the sidelobe structure is optimized. Mismatched filters can

               be designed to minimize the output PSL, minimize the output integrated sidelobe
               level  (ISL)  (sum  of  the  squares  of  all  the  sidelobe  values  of  the  discrete
               correlation of the code and filter, divided by the square of the peak), or to shape
               the output sidelobe response, for instance to enforce particularly low near-in
               sidelobes at the expense of higher distant sidelobes. The filter order L is usually
               larger than the code length. In many cases the design of the mismatched filter
               coefficients  can  be  formulated  as  the  solution  of  a  weighted  least  squares

               problem,  for  which  many  numerical  algorithms  are  available.  Other
                                                          1
               optimization  techniques,  such  as  L   minimization  using  convex  optimization
               algorithms, can also be employed.
                     Figure 4.57 illustrates two examples of mismatched filter design. In both
               cases, the waveform phase code was the same N = 64 MPS biphase code. The

               peak sidelobe of the matched filter output for this length is 4, giving a PSL in dB
               of 20 log (4/64) = –24.1 dB. The ISL for the matched filter is –6.7 dB. The
                          10
               solid  line  in  the  figure  is  the  result  of  a  mismatched  filter  of  length L = 130
               designed to minimize the PSL. The filter impulse response is normalized to have
               the same energy as the code and its matched filter impulse response, namely 64.
               This filter achieves a PSL of –31.4 dB, an 8.3 dB improvement compared to the
               matched filter. The ISL is –9.8 dB, an improvement of about 3.1 dB. However,

               there is now an LPG of 1.11 dB relative to the matched filter.
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