Page 391 - Fiber Optic Communications Fund
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372                                                               Fiber Optic Communications


            The transfer function of the matched filter is

                                                   ∗
                                           H ()= x ()e i+iT b , j = 0, 1
                                            j      j
                                                  ∗
                                                = ̃s ( −  )e i+iT b ,                (8.277)
                                                  j      c
            where  is an arbitrary phase factor. The output of the photodetector j at t = T is
                                                                           b
                                                              2
                                       I (T )= R[|u (T )+ n (T )| ],  j = 0, 1.              (8.278)
                                                        Fj
                                                           b
                                          b
                                                 j
                                                   b
                                       j
            First let us consider the photodetector outputs in the absence of noise. Suppose a bit ‘1’ is transmitted so that
            x(t)= x (t). The output of PD1 is
                   1
                                                              2
                                               I (T )= R[|u (T )| ].                         (8.279)
                                               1  b      1  b
            From Eqs. (8.275) and (8.277), we have
                                                e i  ∞    2        i
                                        u (T )=  2 ∫ −∞  |x ()| d = E e ,              (8.280)
                                                                   1
                                                        1
                                            b
                                         1
                                                            2
                                                  I (T )= RE .                               (8.281)
                                                     b
                                                   1
                                                            1
            For this case, the output of PD0 is
                                                       2
                                            b
                                                   0
                                         0
                                         I (T )= R|u (T )|
                                                     b
                                                       ∞             2
                                                 |  1         ∗     |
                                              = R |      ̃ x ()̃x () d .               (8.282)
                                                                    |
                                                 | 2 ∫ −∞         | |
                                                          1
                                                              0
                                                 |
            Using Parseval’s relations,
                                           ∞                 ∞
                                       1           ∗                ∗
                                                                1
                                      2 ∫ −∞  ̃ x ()̃x ()d =  ∫ −∞  x (t)x (t) dt,   (8.283)
                                              1
                                                   0
                                                                   0
            Eq. (8.282) may be rewritten as
                                                              2
                                               |  T b         |
                                               |         ∗    |
                                           b
                                                     1
                                        0
                                                         0
                                       I (T )= R| |∫  x (t)x (t) dt|
                                               |  0           | |
                                                              2
                                               |  T b        |
                                               |         ∗   |
                                            = R|    s (t)s (t) dt|
                                               |∫            |
                                                     1
                                                         0
                                               |  0          |
                                                                  2
                                               |  T b             |
                                               |                  |
                                            = R|    exp (−i2Δft) dt|
                                               |∫ 0               |
                                               |                  |
                                                                       2
                                               |exp (−iΔfT ) sin (ΔfT )|
                                                                     b
                                                           b
                                            = R |                     |
                                               |         Δf         |
                                               |                      |
                                                   2
                                              Rsin (ΔfT )
                                                         b
                                            =              .                                 (8.284)
                                                   2
                                                   Δf  2
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