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 196
... depends on λ , we have Δλ = λ2 2L ( n - λdn / dλ ) - ( b ) If the group refractive index ( n − λdn / dλ ) is 4.5 for GaAs at 850 nm , what is the mode spacing for a 400 - μm - long laser . 4-15 . For laser structures that have strong ...
... depends on λ , we have Δλ = λ2 2L ( n - λdn / dλ ) - ( b ) If the group refractive index ( n − λdn / dλ ) is 4.5 for GaAs at 850 nm , what is the mode spacing for a 400 - μm - long laser . 4-15 . For laser structures that have strong ...
Page 269
... depends on the carrier ionization rate and on the width of the multiplication region , both of which depend on the applied reverse - bias voltage Va . This gain can be described by the empirical relationship47 Мо = IM Ip = 1 1 Va - IMRM ...
... depends on the carrier ionization rate and on the width of the multiplication region , both of which depend on the applied reverse - bias voltage Va . This gain can be described by the empirical relationship47 Мо = IM Ip = 1 1 Va - IMRM ...
Page 429
... depends on the optical input intensity . As the input signal level is increased , excited carriers ( electron - hole pairs ) are depleted from the active region . When there is a sufficiently large optical input power , further ...
... depends on the optical input intensity . As the input signal level is increased , excited carriers ( electron - hole pairs ) are depleted from the active region . When there is a sufficiently large optical input power , further ...
Contents
Overview of Optical Fiber Communications | 1 |
Structures Waveguiding and Fabrication | 25 |
Structures Waveguiding and Fabrication | 26 |
Copyright | |
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analog attenuation avalanche photodiode band bandwidth cable carrier channel cladding communication components connector core coupler coupling data rate dB/km density detector device dispersion EDFA effects electric emission emitting energy equation example factor fiber end fiber optic FIGURE frequency function gain given by Eq glass graded-index fiber IEEE InGaAs input laser diode lasing layer length Lett light Lightwave Tech loss material Mb/s modal modal noise modes modulation multimode fibers multiplexing n₁ node numerical aperture operating optical amplifiers optical fiber optical output optical power optical signal optical source output power parameter percent photodetector photon pin photodiode power level propagation pulse quantum efficiency Quantum Electron radius range receiver refractive index region semiconductor shown in Fig signal-to-noise ratio single-mode fibers spectral width splice star coupler step-index fiber temperature transmission transmitted values voltage wave wavelength