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Optical Modulators and Modulation Schemes                                          157


           4.6.2.3  Electroabsorption Modulator (EAM)
           Electroabsorption refers to the dependence of the absorption coefficient of a semiconductor on the applied
           electric field. The band gap of a semiconductor decreases as the applied field increases. Consider an optical
           carrier with frequency f < E ∕h, where E g0  is the band gap in the absence of the applied electric field. Let
                                  g0
                             c
           the driving voltage V(t) vary from 0 to V volts, as shown in Fig. 4.17. When V(t)= 0, the photon energy
                                            0
           is less than the band gap and the optical carrier is not absorbed. When V(t)= V , the band gap decreases.
                                                                            0
           Now the photon energy could be larger than the band gap and the optical carrier is absorbed, which generates
           electron–hole pairs. Thus, the information in the electrical domain is translated into the optical domain.
           Fig. 4.18 shows the typical dependence of the absorption coefficient on the wavelength. Suppose the carrier
           wavelength is  .Let  and  be the absorption coefficients at V(t)= 0 and V(t)= V , respectively. If L is
                                   1
                                                                                0
                             0
                       0
           the length of the modulator, the optical power exiting the modulator is
                                      {
                                         P max  = P exp (− L)  when V(t)= 0
                                                0
                                                        0
                                 P out  =                                                   (4.71)
                                         P   = P exp (− L)  when V(t)= V
                                          min   0      1                 0
                                                            V(t)
                                                  V(t)
                                                           V 0
                                                                             t
                              Light signal       EA
                                              modulator


                                                           Field  envelope

                                                                            t

                                   Figure 4.17  Amplitude modulation using an EAM.







                                  Absorption coefficient  α 1  V = 0  V = V 0










                                   α 0
                                                                 Wavelength, λ
                                                   λ 0
                           Figure 4.18  Typical dependence of absorption coefficient on wavelength.
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