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Light Sources and Transmitters



                                                                 Light Sources and Transmitters  89


                     TABLE 6.1. Some LED and Laser Diode Material Mixtures
                     and Their Characteristics
                     Material    Wavelength range, nm  Bandgap energies, eV
                     GaAs               900               1.4
                     GaAlAs           800–900             1.4–1.55
                     InGaAs          1000–1300           0.95–1.24
                     InGaAsP          900–1700           0.73–1.35


                      mixtures together with their operating wavelength range and approximate
                      bandgap energies. Alloys consisting of three elements are called ternary com-
                      pounds, and four-element alloys are known as quaternary compounds. A specific
                      operating wavelength can be selected for AlGaAs, InGaAs, and InGaAsP devices
                      by varying the proportions of the constituent atoms. Thus devices can be tai-
                      lored to emit at a selected wavelength in the 780- to 850-nm band or in any of
                      the other transmission bands ranging from 1280 to 1675nm for glass fibers.

          6.1.2. Spectral output width
                      A major difference between light sources is the spectral width of their light out-
                      put. This is an important factor when one is choosing an optical source since, as
                      Chap. 4 notes, signal spreading in an optical fiber due to chromatic dispersion is
                      directly proportional to the wavelength band over which a source emits light.
                      Recall that chromatic dispersion occurs since each wavelength in a light signal
                      travels at a slightly different velocity. This effect progressively smears out an opti-
                      cal signal as it travels along a fiber. Consequently in order to send a high-speed
                      signal (consisting of very narrow light pulses) over long distances, the source needs
                      to emit light within as narrow a spectral width as possible. This can be done only
                      with laser diodes. An LED has spectral widths ranging from 30nm at a central
                      wavelength of 850nm to around 120nm at a 1550-nm central wavelength. Laser
                      diodes, on the other hand, can have spectral widths of a few picometers (10  3  nm)
                      at 1550nm. For a laser diode the spectral width is referred to as the linewidth.

                        Example Consider a fiber that has a chromatic dispersion D   2ps/(km·nm). Sup-
                        pose we want to send a 10-Gbps signal over this fiber. At 10 Gbps the pulse widths are
                        1/(10Gbps)   100ps. If 20 percent pulse spreading is tolerable, then this data rate has
                        an allowable spread of 20ps before adjacent pulses overlap too much. Then if we use
                        an inexpensive laser source with a 5-nm linewidth, this signal can travel only 2km
                        before the pulse overlap limit is reached. For a high-quality laser with a 0.05-nm
                        linewidth, the chromatic dispersion distance limit is 2000km.


          6.1.3. Modulation speed
                      Direct modulation is the process of using a varying electric signal to change the
                      optical output level of a device. The term modulation speed refers to how fast a


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