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 110
... becomes V ( t ) = + Ꭱ , 4k01 [ 4k0 Rin ' B ' R2A2 + R2 + ( 2m ) / + ( 2πC ) 2 ( B ′ ) 3 ] 4k @ 3 -R2A2 3 g ( 4.29 ) The value in ( 4.29 ) can be decreased by an increase of resistance R1 , but an integration effect will appear again ...
... becomes V ( t ) = + Ꭱ , 4k01 [ 4k0 Rin ' B ' R2A2 + R2 + ( 2m ) / + ( 2πC ) 2 ( B ′ ) 3 ] 4k @ 3 -R2A2 3 g ( 4.29 ) The value in ( 4.29 ) can be decreased by an increase of resistance R1 , but an integration effect will appear again ...
Page 183
... becomes equal to sech ( 1 ) = 0.65 . The relationship between the peak value , u 。, of the electrical field and the pulse width , to , can be obtained using ( 7.3b ) and ( 7.3c ) , that is , uo = 1 1/2 ( - λβό πης ( 7.11 ) It is more ...
... becomes equal to sech ( 1 ) = 0.65 . The relationship between the peak value , u 。, of the electrical field and the pulse width , to , can be obtained using ( 7.3b ) and ( 7.3c ) , that is , uo = 1 1/2 ( - λβό πης ( 7.11 ) It is more ...
Page 266
... becomes dominant . The Raman cross - talk effect imposes the most severe restrictions on transmitter power if the number of channels becomes higher than several hundred . Several methods have been proposed so far to compensate for the ...
... becomes dominant . The Raman cross - talk effect imposes the most severe restrictions on transmitter power if the number of channels becomes higher than several hundred . Several methods have been proposed so far to compensate for the ...
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