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Electromagnetics and Optics                                                         31


                                                y
                                                      a
                                              a y
                                                    θ
                                                             x
                                                     a x
                                                                              √
                                                                                 2
                                                                                    2
           Figure 1.28  The x-and y-polarization components of a plane wave. The magnitude is |a| =  a x + a y and the angle is
                −1
            = tan (a ∕a ).
                   y  x
           1.11  Polarization of Light

           So far we have assumed that the electric and magnetic fields of a plane wave are along the x- and y-directions,
           respectively. In general, an electric field can be in any direction in the x–y plane. This plane wave propagates
           in the z-direction. The electric field intensity can be written as
                                               E = A x + A y,                              (1.188)
                                                          y
                                                    x
                                          A = a exp [i(t − kz)+ i ],                   (1.189)
                                                                x
                                           x
                                               x
                                          A = a exp [i(t − kz)+ i ],                   (1.190)
                                               y
                                           y
                                                                y
           where a and a are amplitudes of the x- and y-polarization components, respectively, and  and  are the
                       y
                 x
                                                                                    x
                                                                                          y
           corresponding phases. Using Eqs. (1.189) and (1.190), Eq. (1.188) can be written as
                                          E = a exp [i(t − kz)+ i ],                   (1.191)
                                                               x
                                            a = a x + a exp (iΔ)y,                       (1.192)
                                                     y
                                                x
           where Δ =  −  . Here, a is the complex field envelope vector. If one of the polarization components
                       y
                           x
           vanishes (a = 0, for example), the light is said to be linearly polarized in the direction of the other polarization
                   y
           component (the x-direction). If Δ = 0or , the light wave is also linearly polarized. This is because the
                                                                               −1
                                       2
                                   2
           magnitude of a in this case is a + a and the direction of a is determined by  =±tan (a ∕a ) with respect
                                   x   y                                          y  x
           to the x-axis, as shown in Fig. 1.28. The light wave is linearly polarized at an angle  with respect to the x-axis.
           A plane wave of angular frequency  is characterized completely by the complex field envelope vector a.It
           can also be written in the form of a column matrix, known as the Jones vector:
                                                 [          ]
                                                      a x
                                              a =            .                             (1.193)
                                                  a exp (iΔ)
                                                   y
           The above form will be used for the description of polarization mode dispersion in optical fibers.
           Exercises
            1.1 Two identical charges are separated by 1 mm in vacuum. Each of them experience a repulsive force
                of 0.225 N. Calculate (a) the amount of charge and (b) the magnitude of electric field intensity at the
                location of a charge due to the other charge.
                                       7
                (Ans: (a) 5 nC; (b) 4.49 ×10 N/C.)
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