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Optical Amplifiers



                                                                          Optical Amplifiers  179















                      Figure 11.3. Simple diagram of a semiconduc-
                      tor optical amplifier (SOA).


                        As in the operation of laser diodes, external current injection is the pumping
                      method used to create the population inversion needed for the operation of the
                      gain mechanism in semiconductor optical amplifiers.
                        Whereas the end facets of a laser diode have a high reflectivity (more than
                      99 percent) so that the optical signal can oscillate in the lasing cavity, a facet
                      reflectivity of less than 0.01 percent is necessary in an SOA to prevent oscilla-
                      tions. Typically this is achieved through a combination of antireflection coat-
                      ings and angular end faces; that is, the optical waveguide in the SOA is tilted
                      by a few degrees with respect to the facet. Any light reflected from the facet
                      thus will propagate away from the waveguide.

          11.3.2.  Basic SOA parameters
                      The five basic parameters used to characterize SOAs are gain, gain bandwidth,
                      saturation power, noise figure, and polarization sensitivity. The following
                      describes the characteristics of these parameters.
                      ■ Gain. Figure 11.4 illustrates the dependence of the gain on the input power
                       for three different bias conditions for a representative SOA. In the example
                       here, at a bias current of 300mA the zero-signal gain (or small-signal gain) is
                       G 0  26dB, which is a gain factor of about 400. The curves show that as the in-
                       put signal power is increased, the gain first stays constant near the small-
                       signal level. This flat region is called the unsaturated region of the SOA gain.
                       For higher input powers above this region the gain starts to decrease. The
                       higher power levels are still amplified, but the gain declines as the power is
                       increased. This gain decline is caused by a reduction in carrier density due to
                       high optical input power. After decreasing linearly over a certain range of
                       input powers, the gain finally approaches an asymptotic value of 0dB (a unity
                       gain) for a very high power level.
                      ■ Saturation power. The region in which the gain value declines is called the
                       saturated gain region of the SOA. The point at which the gain is reduced by
                       3dB (a factor of 2) from the unsaturated value is called the saturation power.
                       This is illustrated in Fig. 11.4 where for a 300-mA bias current the saturation


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