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 88
... term stability character and the long - term stability character . Frequency stability is determined by the ratio of the average frequency of the output optical signal and the frequency fluctuations range , Aƒ ( 7 ) , in the considered ...
... term stability character and the long - term stability character . Frequency stability is determined by the ratio of the average frequency of the output optical signal and the frequency fluctuations range , Aƒ ( 7 ) , in the considered ...
Page 176
... term ẞ causes the phase shift of the optical wave , the term ẞ ' is the cause of the pulse delay , while the terms ẞ ” and ẞ ” cause the pulse broadening and the pulse distortion , respectively . The nonlinear term n2 | E | leads to the ...
... term ẞ causes the phase shift of the optical wave , the term ẞ ' is the cause of the pulse delay , while the terms ẞ ” and ẞ ” cause the pulse broadening and the pulse distortion , respectively . The nonlinear term n2 | E | leads to the ...
Page 186
... term influence . The influence of the loss on soliton behavior is stronger and can be analyzed by application of the perturbation method as well . Equation ( 7.4 ) with the included loss term takes the form dq 1 d2q + \ ql3q = −jÃq ...
... term influence . The influence of the loss on soliton behavior is stronger and can be analyzed by application of the perturbation method as well . Equation ( 7.4 ) with the included loss term takes the form dq 1 d2q + \ ql3q = −jÃq ...
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