Page 214 - Photonics Essentials an introduction with experiments
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Optical Fibers and Optical Fiber Amplifiers

          208   Advanced Topics

            The material dispersion of SiO 2 has been measured and is shown in
          Fig. 9.10.
            Estimation of the pulse spreading due to material dispersion can be
          written simply:
                                      M = L(  )M                     (9.19)

          where    is the linewidth of the laser source under modulation.


          Example 9.2
          To illustrate the importance of the role of modulation bandwidth in
          dispersion, consider the pulse broadening of a narrow-line width, sin-
          gle-mode laser operating near 1300 nm, at which the material disper-
          sion is small.
            The line width of a single-mode distributed feedback laser diode is
          typically less than 0.1 nm. Under low-frequency modulation condi-
          tions (e.g., a modulation frequency less than 1 MHz), the broadening
          of a pulse due to material dispersion is
                           M = L(  )M = L(0.1)3 = 0.3 psec/km

          However, at a modulation frequency of 1 MHz, the pulse width itself
                        6
          is already ~10 psec in width. After transmission through 100 km of
          fiber, the intrinsic pulse duration is still four orders of magnitude
          larger than the broadening due to dispersion.
            Now consider a laser modulated at 10 Gbits/sec. The time duration
          of this pulse is approximately :

                                      1
                              t =           = 100 psec
                                         9
                                  (10 × 10 )
            The frequency bandwidth of the pulse is
                                    2
                                f 	    = 2 × 10 10  Hz
                                     t
            The central frequency of the light pulse at 1300 nm is 2.3 × 10 14  Hz.
                                                                    10
          The modulation of the laser broadens the frequency by 2 × 10 /2.3 ×
                        –4
          10 14  	 0.9 × 10 . The wavelength spread of the emission is the same
          percentage, so that    = 0.1 nm. As a result the wavelength broaden-
          ing under modulation is now significant = 0.1 nm + 0.1 nm = 0.2 nm.
            The pulse width broadening is now two times larger than the case
          at 1 MHz or 0.6 psec per km. After 100 km, this results in a broad-
          ening of 60 psec. Remember that the width of the pulse at 10
          Gbits/sec is 100 psec. So dispersion has broadened the signal pulse
          to almost two-thirds more than its allotted bit period. Clearly, this is
          a problem. Some dispersion correction is needed. At the next lower


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