## 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 10

The stimulated Brillouin scattering arises as a consequence of interaction

between the incident optical wave and the acoustic waves , when the

stimulated Brillouin ...

The stimulated Brillouin scattering arises as a consequence of interaction

between the incident optical wave and the acoustic waves , when the

**corresponding**wave vectors are matched . Because of this matching , thestimulated Brillouin ...

Page 36

It can be seen that the sampled values have the normal distributions with the

mean values equal to Sh and - Sh . The

xi – 2x1x2 + xy = xy + x3 = 0 % 1 + oło ( 2 . 75 ) If the power of the local optical ...

It can be seen that the sampled values have the normal distributions with the

mean values equal to Sh and - Sh . The

**corresponding**variance is ( x1 - x2 ) 2 =xi – 2x1x2 + xy = xy + x3 = 0 % 1 + oło ( 2 . 75 ) If the power of the local optical ...

Page 126

92 ) where , and E are the values of the electrical fields of

optical signals , a and B ( B = 1 - a ) are the port - coupling coefficients in the

optical mixer , and E , and E , are the electrical fields of the incoming optical

signal ...

92 ) where , and E are the values of the electrical fields of

**corresponding**outputoptical signals , a and B ( B = 1 - a ) are the port - coupling coefficients in the

optical mixer , and E , and E , are the electrical fields of the incoming optical

signal ...

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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