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 23
... conditions and στ = στ = σε 2 ( 2.32 ) opt 10 ( Sbaw ) exp ( -2 ) = 1 σ2 ( 2.33 ) The condition in ( 2.32 ) is satisfied when the local optical oscillator has power considerably higher than the power of the incoming optical signal . It ...
... conditions and στ = στ = σε 2 ( 2.32 ) opt 10 ( Sbaw ) exp ( -2 ) = 1 σ2 ( 2.33 ) The condition in ( 2.32 ) is satisfied when the local optical oscillator has power considerably higher than the power of the incoming optical signal . It ...
Page 72
... condition that the phase and group velocities of the propagating wave are equal in the wide region of frequencies . Such a condition can be imposed on a line with tranversal electromagnetic ( TEM ) type wave , filled particularly with ...
... condition that the phase and group velocities of the propagating wave are equal in the wide region of frequencies . Such a condition can be imposed on a line with tranversal electromagnetic ( TEM ) type wave , filled particularly with ...
Page 177
... conditions . These conditions concern the optical signal power level , the shape of the signal envelope , the operating wavelength , the optical fiber loss , and so on . Under these conditions , the pulse will preserve its input shape ...
... conditions . These conditions concern the optical signal power level , the shape of the signal envelope , the operating wavelength , the optical fiber loss , and so on . Under these conditions , the pulse will preserve its input shape ...
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