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Channel Multiplexing Techniques                                                    409



           The maximum reach is given by
                                       T g                 1.28 × 10 −9
                            L max  =          =
                                   | |(2NΔf)  22 × 10 −27  × 2 × 128 × 78.125 × 10 6
                                    2
                                 = 925 km.                                                  (9.91)




           9.5  Time-Division Multiplexing
           In the case of frequency-division multiplexing, parallel streams of data are modulated by carriers with differ-
           ent frequencies so that the data spectra do not overlap (see Fig. 9.4). Instead, the parallel streams of data can be
           converted to serial data in such a way that the individual streams do not overlap in time. This type of multiplex-
           ing is known as time-division multiplexing (TDM). Fig. 9.19 illustrates the schematic of a two-channel TDM.
           Let T be the symbol interval of the individual data streams corresponding to a symbol rate of B = 1∕T .
               s                                                                         s      s
           TDM converts the parallel data streams into serial data with two symbols within the symbol interval T ,as
                                                                                             s
           shown in Fig. 9.19. To avoid the overlap in time, the pulse widths should be less than T ∕2. In this example,
                                                                                s
           the total symbol rate is 2B . In general, for an N-channel TDM system, the pulse widths should be less than
                                s
           T ∕N and the total symbol rate is NB .
            s
                                        s
            TDM can be performed in either an electrical or an optical domain. However, as the bit rate increases beyond
           40 Gb/s, if becomes hard to do electrical TDM because of the limitations imposed by high-speed electronics.
           Instead, channels can be multiplexed in the optical domain and such a scheme is known as optical TDM
           (OTDM). Because of the wide bandwidth of optical devices, OTDM can be used to obtain a total bit rate of
           several terabits per seconds.

           9.5.1  Multiplexing

           To realize OTDM, ultra-short laser pulses and delay lines are required [7, 43]. Fig. 9.20 shows a schematic of a
           four-channel OTDM system. A train of ultra-short pulses is split into four branches. Each branch is modulated
           by the electrical data. To avoid the temporal overlap of channels, channel j, j = 1, 2, 3, 4, is delayed by (j − 1)T,
           where T = T ∕4, using a delay line. The delay lines can be realized using fiber segments (see Example 2.5).
                     s
           The output of all branches is combined to obtain a TDM signal.

                                                               Ch. 2  Ch. 2  Ch. 2  Ch. 2
                   Ch. 1                                    Ch. 1  Ch. 1  Ch. 1  Ch. 1


                        T s
                                                               T s
                                                    TDM
                   Ch. 2                                             TDM signal

                        T s



                                    Figure 9.19  Schematic of a two-channel TDM.
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