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 9
These effects will be considered in detail in Chapter 6 ; now we are giving only a
brief review of the nonlinear effects and the conditions for their appearance . The
main nonlinear effects that can appear in optical fibers are : stimulated Raman ...
These effects will be considered in detail in Chapter 6 ; now we are giving only a
brief review of the nonlinear effects and the conditions for their appearance . The
main nonlinear effects that can appear in optical fibers are : stimulated Raman ...
Page 158
1 Stimulated Raman and Stimulated Brillouin Scattering Raman and Brillouin
scattering processes can be explained by application of the quantum radiation
theory . In that theory , these processes are considered to be twostage reactions .
1 Stimulated Raman and Stimulated Brillouin Scattering Raman and Brillouin
scattering processes can be explained by application of the quantum radiation
theory . In that theory , these processes are considered to be twostage reactions .
Page 169
It was found [ 4 - 5 ] that the stimulated Brillouin amplification coefficient in single -
mode optical fiber is over two orders of magnitude larger than the amplification
coefficient for stimulated Raman scattering , that is , Q0 ~ 4 · 10 - 9 cm / W . To ...
It was found [ 4 - 5 ] that the stimulated Brillouin amplification coefficient in single -
mode optical fiber is over two orders of magnitude larger than the amplification
coefficient for stimulated Raman scattering , that is , Q0 ~ 4 · 10 - 9 cm / W . To ...
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Contents
Preface | 5 |
Coherent Optical Receiver Sensitivity | 15 |
Optical Transmitters for Coherent Lightwave Systems | 61 |
Copyright | |
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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 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