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 237
... continuous waves . These waves must have the same frequency and phase as the soliton wave . The employment of optical amplifiers will be described after the analysis of soliton regeneration by continuous - wave injection . When a continuous ...
... continuous waves . These waves must have the same frequency and phase as the soliton wave . The employment of optical amplifiers will be described after the analysis of soliton regeneration by continuous - wave injection . When a continuous ...
Page 239
... continuous wave is not totally absorbed by the soliton pulse . The unabsorbed part of the continuous wave will continue propaga- tion as a linear dispersive wave . This linear dispersive wave does not affect the soliton shape since the ...
... continuous wave is not totally absorbed by the soliton pulse . The unabsorbed part of the continuous wave will continue propaga- tion as a linear dispersive wave . This linear dispersive wave does not affect the soliton shape since the ...
Page 240
... continuous 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 ...
... continuous 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 ...
Contents
Coherent Optical Receiver Sensitivity | 15 |
7 | 37 |
References | 60 |
Copyright | |
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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