Optical Fiber CommunicationsThe third edition of this popular text and reference book presents the fundamental principles for understanding and applying optical fiber technology to sophisticated modern telecommunication systems.. Optical-fiber-based telecommunication networks have become a major information-transmission-system, with high capacity links encircling the globe in both terrestrial and undersea installations. Numerous passive and active optical devices within these links perform complex transmission and networking functions in the optical domain, such as signal amplification, restoration, routing, and switching. Along with the need to understand the functions of these devices comes the necessity to measure both component and network performance, and to model and stimulate the complex behavior of reliable high-capacity networks. |
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Page 78
T . Miya , Y . Terunuma , T . Hosaka , and T . Miyashita , " An ultimate low loss
single mode fiber at 1 . 55 um , ” Electron . Lett . , 15 , 106 - 108 , Feb . 1979 . 33 .
M . Horiguchi and H . Osanai , " Spectral losses of low OH content fibers , ”
Electron ...
T . Miya , Y . Terunuma , T . Hosaka , and T . Miyashita , " An ultimate low loss
single mode fiber at 1 . 55 um , ” Electron . Lett . , 15 , 106 - 108 , Feb . 1979 . 33 .
M . Horiguchi and H . Osanai , " Spectral losses of low OH content fibers , ”
Electron ...
Page 143
M . Born and E . Wolf , Principles of Optics , Pergamon , Oxford , 1965 , p . 189 . 7
. K . H . Yang and J . D . Kingsley , “ Calculation of coupling losses between light
emitting diodes and low loss optical fibers , ” Appl . Opt . , 14 , 288 – 293 , Feb .
M . Born and E . Wolf , Principles of Optics , Pergamon , Oxford , 1965 , p . 189 . 7
. K . H . Yang and J . D . Kingsley , “ Calculation of coupling losses between light
emitting diodes and low loss optical fibers , ” Appl . Opt . , 14 , 288 – 293 , Feb .
Page 238
Assume connector losses at the multiplexer , source , and detector are 1 . 0 dB .
Table P8 - 9 810 0 . 0 835 - 1 . 0 860 - 0 . 5 890 - 1 . 8 Source wavelength ( nm )
Source output ( dBm ) Multiplexer insertion loss ( dB ) Fiber attenuation ( dB / km )
...
Assume connector losses at the multiplexer , source , and detector are 1 . 0 dB .
Table P8 - 9 810 0 . 0 835 - 1 . 0 860 - 0 . 5 890 - 1 . 8 Source wavelength ( nm )
Source output ( dBm ) Multiplexer insertion loss ( dB ) Fiber attenuation ( dB / km )
...
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Contents
Structures and Waveguiding | 12 |
Signal Degradation in Optical Fibers | 48 |
Optical Sources | 80 |
Copyright | |
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absorption active addition amplifier angle applications approximately arise assume attenuation avalanche band bandwidth becomes bias cable carrier characteristics cladding communication components condition consider constant core coupling defined density depends detector determined device dispersion distance distortion effects efficiency electric Electron emitting energy equal equation example expression factor field Figure frequency function gain given gives glass graded-index guided IEEE important increases input laser diodes length less light limit loss material measured mechanical method modes modulation noise occurs operating optical fiber optical power optical source output parameter percent photodetector photodiode photon propagation pulse quantum range ratio receiver referred reflection region respectively response rise shown in Fig signal spectral surface technique temperature transmission transmitter values various voltage wave waveguide wavelength width York