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228                                                               Fiber Optic Communications


            mode dispersion (PMD) in an electrical domain. In the case of coherent detection, the detection process is
            linear–the complex optical field envelope is linearly translated into an electrical domain and, therefore, the
            inverse fiber transfer function can be realized using DSP to compensate for dispersion and PMD. (ii) With
            coherent detection, higher spectral efficiencies can be realized using multi-level modulation formats that make
            use of both amplitude and phase modulation.


            5.6.1   Single-Branch Coherent Receiver
            In this section, we assume that the polarization of the received signal is perfectly aligned with that of the local
            oscillator (LO), and we use scalar notation. The polarization effects are considered in Section 5.6.5. Let the
            transmitted signal be
                                             q (t)= A s(t) exp (−i t),                      (5.85)
                                                    T
                                                                c
                                              T
                                                                                   2
            where s(t) is the complex field envelope,  is the frequency of the optical carrier, and A is the peak trans-
                                               c                                   T
            mitter power. Let us assume a perfect optical channel that introduces neither distortion nor noise. However,
            the phase of the optical carrier changes due to propagation, and the field amplitude may be attenuated. Let
            the received signal be
                                           q (t)= A s(t) exp [−i( t +  )]                 (5.86)
                                            r     r          c    c
            and the local oscillator output be
                                         q  (t)= A  exp [−i(  t +   )],                   (5.87)
                                          LO      LO        LO    LO
            where A 2  = P LO  is the LO power, and  LO  is the phase. These two signals are combined using a 3-dB
                   LO
                                                                    1
            coupler and pass through a photodetector (PD), as shown in Fig. 5.30 . The photocurrent is proportional to
            the absolute square of the incident optical field. Therefore, the photocurrent is
                                              √
                          I(t)= R|[q (t)+ q      2
                                  r     LO  (t)]∕ 2|
                               R       2       2
                             =  {|A s(t)| + |A LO | + 2A A  Re {s(t) exp [−i( t +  −  LO )]}}  (5.88)
                                                                      IF
                                                    r LO
                                                                            c
                                   r
                               2
            where
                                                  =  −  LO                              (5.89)
                                                  IF
                                                        c
                                              Received       [q (t) + q (t)]/  2
                                                              r
                                                                   LO
                                  q (t)         signal
                                   T
                              Tx        Optical        C                 I(t)  ESP
                                        channel  q (t)
                                                 r
                                                                   PD
                                                        q (t)
                                                         LO
                                                      LO
            Figure 5.30  Block diagram of a single-branch coherent receiver. Tx = transmitter, LO = local oscillator, C = 3-dB
            coupler, PD = photo-detector, ESP = electrical signal processor.
            1  An unbalanced directional coupler can be used to combine the signals to maximize SNR [74]. In this section, a 3-dB coupler is used
            for simplicity.
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