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Light Sources and Transmitters



                                                                 Light Sources and Transmitters  91























                      Figure 6.3. Typical relationship between the optical
                      signal generated by an LED and the drive current.


                      operate around 50- to 100-mA drive currents and require a bias voltage of
                      around 1.5 V. As shown in Fig. 6.3, to send a digital signal, the drive current can
                      simply turn the LED on during a 1 pulse (current I   I 1 produces power level
                      P 1 ) and off during a 0 pulse (current I   0).
                        The light that is emitted during electron-hole recombination can go in all
                      directions. Therefore engineers have varied the device geometry and internal
                      structure in different ways to confine and guide the light so it can be coupled
                      efficiently into a fiber (see the text below on photon and carrier confinement for
                      details). Even so, LEDs have fairly broad emission patterns. Because of this
                      they are used mainly with multimode fibers, since they couple too little light
                      into single-mode fibers. Two LED configurations are the surface-emitting and
                      edge-emitting structures.


          6.2.2. Surface emitters
                      In the surface emitter a circular metal contact defines the active region in which
                      light is generated, as Fig. 6.4 shows. The contact is nominally 50µm in diameter.
                      To couple the light into a fiber, first a well is etched into the substrate on which
                      the device is fabricated. A multimode fiber that has a core diameter of 50µmor
                      larger then can be brought close to the region where the light is generated and
                      can be cemented in place. The light emission pattern is isotropic (also called
                      lambertian), which means it is equally bright when viewed from any direction.
                      Since the emission area and the fiber core area are the same, most of the emit-
                      ted light will shine on the fiber core end face. However, not all the light will be
                      coupled into the fiber since it has a limited numerical aperture (i.e., a limited
                      light acceptance cone), as Fig. 6.5 shows. Chapter 7 presents more details on
                      power coupling factors.


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