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 11
The optical solitons , or the optical pulses with characteristic shape , can
propagate through an optical fiber with preserving ... the carrier wavelength , the
pulse width , and the optical - fiber dispersion characteristics at the carrier
wavelength .
The optical solitons , or the optical pulses with characteristic shape , can
propagate through an optical fiber with preserving ... the carrier wavelength , the
pulse width , and the optical - fiber dispersion characteristics at the carrier
wavelength .
Page 176
To estimate the extent of the pulse spreading and pulse distortion at the output
end of the optical fiber , the definition equations for the propagation constant and
the group velocity should be used . The group velocity , Vg , is given by do Ug ...
To estimate the extent of the pulse spreading and pulse distortion at the output
end of the optical fiber , the definition equations for the propagation constant and
the group velocity should be used . The group velocity , Vg , is given by do Ug ...
Page 184
Hence , only one soliton is to be generated for the hyperbolic secant shape of the
input pulse having 1 - ps width and 1 . 6 - W peak power . This conclusion is valid
in the absence of loss at the wavelength 1 = 1 . 3 um . Only one soliton will be ...
Hence , only one soliton is to be generated for the hyperbolic secant shape of the
input pulse having 1 - ps width and 1 . 6 - W peak power . This conclusion is valid
in the absence of loss at the wavelength 1 = 1 . 3 um . Only one soliton will be ...
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Contents
Preface | 5 |
Coherent Optical Receiver Sensitivity | 15 |
Optical Transmitters for Coherent Lightwave Systems | 61 |
Copyright | |
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