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 117
60 ) ( 4 . 60 ) Then , ( 4 . 59 ) can be transformed to dølt - dt de d Kd h ( t – u ) [ sin
« ( u ) + ne ( u ) ] du ( 4 . 61 ) Jo When the noise at the input of the PLL is a
stationary Gaussian process , the equivalent filtrated noise will be a Gaussian
process ...
60 ) ( 4 . 60 ) Then , ( 4 . 59 ) can be transformed to dølt - dt de d Kd h ( t – u ) [ sin
« ( u ) + ne ( u ) ] du ( 4 . 61 ) Jo When the noise at the input of the PLL is a
stationary Gaussian process , the equivalent filtrated noise will be a Gaussian
process ...
Page 120
The evaluation is considerably simplified with the assumption that the noise at
the input of the PLL has the nature of white noise with the constant value of
spectral power density ( equal to 2vo ) . In such a way , the variance of phase
difference ...
The evaluation is considerably simplified with the assumption that the noise at
the input of the PLL has the nature of white noise with the constant value of
spectral power density ( equal to 2vo ) . In such a way , the variance of phase
difference ...
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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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 integral 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