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Optical Fiber Transmission                                                          53




                                                        1
                                                       0.8
                                                       0.6
                                                       0.4
                                                       0.2
                                                        0
                                                      –0.2
                                                      –0.4
                                                      –0.6
                                                      –0.8
                                                       –1
                                                           –1      –0.5     0       0.5      1

                     Figure 2.21 Optical field and power distributions of LP mode. V = 10.3and b = 0.456.
                                                              22
           In analogy with a 1-dimensional plan wave (Section 1.6.1), the phase speed of this mode can be written as
                                                       
                                                    =  .                                  (2.72)
                                                       
           The phase speed of an electromagnetic wave propagating in a uniform medium of refractive index n  is
                                                                                          eff
                                                       c
                                                   =   .                                  (2.73)
                                                      n
                                                       eff
           Combining Eqs. (2.72) and (2.73), we find
                                                  
                                               =  n eff  = k n .                          (2.74)
                                                         0 eff
                                                  c
           Thus, n  can be interpreted as the effective index “seen” by the mode with propagating constant . Guided
                 eff
           modes occur if k n < < k n or n < n  < n .
                        0 2      0 1    2   eff  1
           2.4.4  2-Dimensional Planar Waveguide Analogy
           Consider a 2-D planar waveguide as shown in Fig. 2.22. Let
                                               {
                                                  n 1  for  |x| < d∕2
                                          n(x)=
                                                  n 2  otherwise













                                    Figure 2.22 A 2-dimensional planar waveguide.
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