Page 462 - Fundamentals of Radar Signal Processing
P. 462

(6.38)

               Expanding the exponent in Eq. (6.38) gives











                                                                                                       (6.39)

               where ϕ is the unknown but fixed phase of the inner product                 .

                     Notice that p (y|H ,θ) does not depend on θ after all (not surprising since
                                           0
                                     y
               there is no target present in this case to present an unknown phase), so it is not
               necessary  to  apply Eq. (6.37).  However,  in p (y|H1)  the  dependence  on θ  is
                                                                        y
               explicit. Assuming a uniform random phase, defining θ′  = ϕ  – θ, and applying
               Eq. (6.37) under H  gives
                                     1







                                                                                                       (6.40)

               Equation (6.40) is a standard integral. Specifically, integral 9.6.16 in Olver et
               al. (2010) is





                                                                                                       (6.41)


               where I (z) is the modified Bessel function of the first kind. Using this result and
                        0
               properties of the cosine function, Eq. (6.40) becomes






                                                                                                       (6.42)

               The log-LRT now becomes
   457   458   459   460   461   462   463   464   465   466   467