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 180
... pulse is present at the photodetector in that time slot . Ideally the output signal tout ( 1 ) would always exceed the threshold voltage when a 1 is present and would be less than the threshold when no pulse ( a 0 ) was sent . In actual ...
... pulse is present at the photodetector in that time slot . Ideally the output signal tout ( 1 ) would always exceed the threshold voltage when a 1 is present and would be less than the threshold when no pulse ( a 0 ) was sent . In actual ...
Page 194
... pulse energy y as a function of the gaussian pulse shape param- eter a . - bit error rate ) as a function of the fraction of pulse energy 1 y that has spread outside of the bit period T. For a given value of y we read the corresponding ...
... pulse energy y as a function of the gaussian pulse shape param- eter a . - bit error rate ) as a function of the fraction of pulse energy 1 y that has spread outside of the bit period T. For a given value of y we read the corresponding ...
Page 250
... pulse response pout ( t ) of the fiber can be calculated through the convolution ( denoted by * ) of the input pulse pin ( t ) and the power impulse response function h ( t ) of the fiber . The period T between the input pulses should ...
... pulse response pout ( t ) of the fiber can be calculated through the convolution ( denoted by * ) of the input pulse pin ( t ) and the power impulse response function h ( t ) of the fiber . The period T between the input pulses should ...
Contents
Structures and Waveguiding | 12 |
Signal Degradation in Optical Fibers | 48 |
Optical Sources | 80 |
Copyright | |
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Common terms and phrases
absorption amplifier angle Appl attenuation avalanche photodiode band gap bandwidth Bell Sys bias cable carrier Chap cladding coefficient communication systems components connector coupler coupling coupling loss data rate dB/km decibels density detector device distortion electric electromagnetic emission emitting energy equation fiber core fiber end fiber optic Figure frequency function given by Eq glass fibers graded-index fiber IEEE Trans input laser diodes layer Lett lifetime light source loss material dispersion measured method modal modulation multimode fibers n₁ n₂ numerical aperture operating optical output optical power optical signal optical source optical waveguide output power parameter percent photodetector photon pin photodiode preform propagation quantum efficiency radiation radius ratio receiver recombination refractive index refractive-index refractive-index profile semiconductor shown in Fig silica single-mode spectral width splice star coupler step-index fiber surface T-coupler technique temperature thermal noise transmitter values voltage wave wavelength