Coherent and Nonlinear Lightwave CommunicationsThis is a practical source on recent developments in coherent and nonlinear lightwave communications. The book systematically presents up-to-date explanations of all the relevant physical principles and recent research in this emerging area. Providing an unparallelled engineering-level treatment (with 700 equations), this reference also describes the progression of coherent and nonlinear technology from yesterday's experimental field to today's practical applications tool. This work is intended as a tool for research telecommunication engineers, applications engineers working with broadband telecom systems and networks, and postgraduate students. |
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Page 71
... wave vector with the intensity k = 2π / λ . The module of the wave vector in the crystal , having the refractive index n , is k = 2πn / λ . Hence , the initial phase of the wave is changed due to the changes in the refractive index in ...
... wave vector with the intensity k = 2π / λ . The module of the wave vector in the crystal , having the refractive index n , is k = 2πn / λ . Hence , the initial phase of the wave is changed due to the changes in the refractive index in ...
Page 239
... wave and the soliton carrier must be equal . Hence , if the continuous wave with amplitude E6 is periodically injected into the optical fiber at distances where the soliton amplitude decreases by the factor E , the original soliton ...
... wave and the soliton carrier must be equal . Hence , if the continuous wave with amplitude E6 is periodically injected into the optical fiber at distances where the soliton amplitude decreases by the factor E , the original soliton ...
Page 240
... wave is expected to preserve its initial phase , so there is a possibility for mutual elimination of unused parts of continuous waves . If the next continuous wave with frequency w = and phase = + σo is injected at the point where the ...
... wave is expected to preserve its initial phase , so there is a possibility for mutual elimination of unused parts of continuous waves . If the next continuous wave with frequency w = and phase = + σo is injected at the point where the ...
Contents
Optical Transmitters for Coherent Lightwave Systems | 3 |
Coherent Optical Receiver Sensitivity | 15 |
61 | 31 |
Copyright | |
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amplification coefficient amplitude Brillouin scattering channels Chapter characteristics coherent detection coherent lightwave system coherent optical receiver components corresponding detection scheme digit interval dispersion DPSK electric field energy equal equation erbium-doped fiber amplifiers error probability evaluated Figure filter frequency shift Gaussian Hence heterodyne detection homodyne detection IEEE IEEE/OSA incoming optical signal influence input laser amplifiers length Lett lightwave communications lightwave systems Lightwave Techn loss modulating signal multichannel nonlinear effects nonlinear lightwave system optical amplifiers optical oscillator optical power optical transmitter optical-fiber parameters phase modulation phase noise phase shift photodetector photodiode photons polarization propagation PSK signals pump signal R₁ Raman amplification Raman amplifiers ratio realization receiver sensitivity refractive index resonator scattered signal self-phase modulation semiconductor laser signal power single-mode optical fiber soliton pulses soliton regime spectral linewidth spontaneous emission stimulated Raman scattering term thermal noise transmission system variance voltage width