## 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 81

The

The

**function**of the instantaneous frequency fluctuations is defined as 1 dan fu ( t ) = 27 dt ( 3.56 ) so , the corresponding power spectral density is SAS ) = lim ; < F : ( S ) F. ( S ) > ( 3.57 ) T - 700 The**function**F ( f ) is the ...Page 115

Thus , the Laplace transform of the phase difference

Thus , the Laplace transform of the phase difference

**function**becomes S Φ ( s ) 01 ( s ) s + K , K , H ( s ) ( 4.51 ) The Laplace transform of the VCO instantaneous phase is 02 ( s ) KK HS ) Φ , ( s ) s + K , K H ( ) ( 4.52 ) The ...Page 277

( D.5 ) According to the rule for transformation of joined probability distribution

( D.5 ) According to the rule for transformation of joined probability distribution

**functions**( 5 ) , the following ... ( D.6 ) Since z = r cos w and y = r sing ( D.7 ) the joined distribution**function**takes the form 1 wnlr , ) = 2πσ2 ...### What people are saying - Write a review

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### Contents

Preface | 5 |

Coherent Optical Receiver Sensitivity | 15 |

Optical Transmitters for Coherent Lightwave Systems | 61 |

Copyright | |

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