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 152
Gerd Keiser. Current gain large gain - bandwidth products . As shown in Fig . 6-6 , of all the materials examined so far , 16-34 only silicon has a significant difference between electron and hole ionization rates . The multiplication M ...
Gerd Keiser. Current gain large gain - bandwidth products . As shown in Fig . 6-6 , of all the materials examined so far , 16-34 only silicon has a significant difference between electron and hole ionization rates . The multiplication M ...
Page 161
... gain is greater than the average gain squared . That is , if m denotes the statistically varying gain then 2 ( m2 ) > ( m ) 2 = M2 ( 6-31 ) where the symbols ( ) denote an ensemble average and ( m ) = M is the average carrier gain ...
... gain is greater than the average gain squared . That is , if m denotes the statistically varying gain then 2 ( m2 ) > ( m ) 2 = M2 ( 6-31 ) where the symbols ( ) denote an ensemble average and ( m ) = M is the average carrier gain ...
Page 163
... Gain 103 Figure 6-14 Variation of the electron excess noise factor F , as a function of the electron gain for various values of the effective ionization rate ratio keff . ( Reproduced with permission from Webb , McIntyre , and Conradi ...
... Gain 103 Figure 6-14 Variation of the electron excess noise factor F , as a function of the electron gain for various values of the effective ionization rate ratio keff . ( Reproduced with permission from Webb , McIntyre , and Conradi ...
Contents
Structures and Waveguiding | 12 |
Signal Degradation in Optical Fibers | 48 |
Optical Sources | 80 |
Copyright | |
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absorption amplifier angle 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 silicon single-mode spectral width splice star coupler step-index fiber surface T-coupler technique temperature thermal noise transmitter values voltage wave wavelength