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 67
... electric field is absent . In the presence of the electric field , the cross - sectional area is an ellipse with the semi - axes 1 1 nx = √a10 - г63E ≈ no + 2når63E ny ' = 1 Va10 + r63E 1 no – zn3r63E ( 3.19 ) ( 3.20 ) Equations ...
... electric field is absent . In the presence of the electric field , the cross - sectional area is an ellipse with the semi - axes 1 1 nx = √a10 - г63E ≈ no + 2når63E ny ' = 1 Va10 + r63E 1 no – zn3r63E ( 3.19 ) ( 3.20 ) Equations ...
Page 73
... electric field . If the light propagates in the y direction , and the electric field vector takes the x - axis position , the following relation is valid : Δυτ C г6зnE 2 ( 3.34 ) where E , is the z - coordinate component of the external ...
... electric field . If the light propagates in the y direction , and the electric field vector takes the x - axis position , the following relation is valid : Δυτ C г6зnE 2 ( 3.34 ) where E , is the z - coordinate component of the external ...
Page 74
... electric field , rather than a magnetic field . The split of the spectral line and the frequency shift are proportional to the intensity of the electric field . The linear Stark effect is characterized by linear dependence of the ...
... electric field , rather than a magnetic field . The split of the spectral line and the frequency shift are proportional to the intensity of the electric field . The linear Stark effect is characterized by linear dependence of 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