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Light Sources and Transmitters



          94  Chapter Six




















































          Figure 6.7. (a) Cross-section (not to scale) of a GaAlAs light emitter. Here x   y to provide both carrier
          confinement and optical guiding. (b) Energy band diagram showing the active region and the electron
          and hole confinement barriers. (c) Variations in the refractive index of the layers.

                        Laser Action The term laser actually is an acronym for the phrase “light amplifica-
                        tion by stimulated emission of radiation.” So what is stimulated emission of radiation
                        and how does it result in light amplification? First, let us look at the possible photon
                        emission and absorption processes shown in Fig. 6.8 for a two-level atomic system. An
                        electron can move from an energy level E 1 in the valence band (called the ground
                        state) to a higher state (called an excited state) at energy level E 2 in the conduction
                        band either by being pumped externally to that level or by absorbing the energy hν 12
                        from a passing photon. The latter process is called stimulated absorption. In either
                        case, an excited electron then can return to the ground state either spontaneously or


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