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Optical Communication Systems Overview



                                                        Optical Communication Systems Overview  23


                      significant attenuation and distortion. Glass is an obvious material for such
                      applications. The earliest known glass was made around 2500  B.C., and glass
                      already was drawn into fibers during the time of the Roman Empire. However,
                      such glasses have very high losses and are not suitable for communication appli-
                      cations. One of the first known attempts of using optical fibers for communication
                      purposes was a demonstration in 1930 by Heinrich Lamm of image transmission
                      through a short bundle of optical fibers for potential medical imaging. However,
                      no further work was done beyond the demonstration phase, since the techno-
                      logy for producing low-loss fibers with good light confinement was not yet
                      mature.
                        Further work and experiments on using optical fibers for image transmission
                      continued, and by 1960 glass-clad fibers had an attenuation of about 1dB/m.
                      This attenuation allowed fibers to be used for medical imaging, but it was still
                      much too high for communications, since only 1 percent of the inserted optical
                      power would emerge from the end of a 20-m-long fiber. Optical fibers attracted
                      the attention of researchers at that time because they were analogous in theory
                      to plastic dielectric waveguides used in certain microwave applications. In 1961
                      Elias Snitzer published a classic theoretical description of single-mode fibers
                      with implications for information transmission use. However, to be applicable
                      to communication systems, optical fibers would need to have a loss of no more
                      than 10 or 20dB/km (a power loss factor of 10 to 100).
                        In the early 1960s when Charles Kao was at the Standard Telecommunication
                      Laboratories in England, he pursued the idea of using a clad glass fiber for an
                      optical waveguide. After he and George Hockman painstakingly examined the
                      transparency properties of various types of glass, Kao made a prediction in 1966
                      that losses of no more than 20dB/km were possible in optical fibers. In July
                      1966, Kao and Hockman presented a detailed analysis for achieving such a loss
                      level. Kao then went on to actively advocate and promote the prospects of fiber
                      communications, which generated interest in laboratories around the world to
                      reduce fiber loss. It took 4 years to reach Kao’s predicted goal of 20dB/km, and
                      the final solution was different from what many had expected.
                        To understand the process of making a fiber, consider the schematic of a typ-
                      ical fiber structure, shown in Fig. 2.1. A fiber consists of a solid glass cylinder
                      called the core. This is surrounded by a dielectric cladding, which has a different
                      material property from that of the core in order to achieve light guiding in the
                      fiber. Surrounding these two layers is a polymer buffer coating that protects the











                      Figure 2.1. A typical fiber structure consists of a core,
                      a cladding, and a buffer coating.


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