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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Results 1-3 of 72
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
Coherent Optical Receiver Sensitivity | 15 |
7 | 37 |
References | 60 |
Copyright | |
10 other sections not shown
Common terms and phrases
according amplifier amplitude applied assumed bandwidth becomes carrier caused channels Chapter characteristics coefficient coherent optical receiver Communications components condition considered constant continuous wave corresponding defined density depends described detection scheme determined difference direct dispersion distance distribution effect Electron emission energy equal equation Erbium error probability evaluated expressed factor Figure filter frequency function gain given Hence heterodyne homodyne IEEE/OSA incoming increase influence input laser length light lightwave systems Lightwave Techn limit loss means methods mode modulation noise nonlinear obtained operation optical amplifiers optical fiber optical oscillator optical power optical receiver optical signal output parameters phase photodiode photons polarization possible practical presents propagation pulse pump Quantum Raman ratio realization referent region resonator respectively scattering semiconductor laser shift soliton spectral spectral linewidth spontaneous stimulated takes term transmission variance wave wavelength