## 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. |

### From inside the book

Results 1-3 of 54

Page 79

Thus , the monomode electromagnetic wave will be amplified by being passed

through the medium with imposed inverse population . This process can be

described by the equation for the radiated photon

f12 ) ...

Thus , the monomode electromagnetic wave will be amplified by being passed

through the medium with imposed inverse population . This process can be

described by the equation for the radiated photon

**density**n , or am = A12N2 + 0 (f12 ) ...

Page 138

Thus , if the modulating signal in the considered Mth channel is s ( t ) = my cos (

27ft + $ M ) and the corresponding power spectral

power spectral

Thus , if the modulating signal in the considered Mth channel is s ( t ) = my cos (

27ft + $ M ) and the corresponding power spectral

**density**function is S , ( f ) , thepower spectral

**density**of the total current signal , in , can be expressed as ...Page 301

... Modulation Phase noise ASK signals and , 27 - 29 defined , 76 DPSK signals

and , 56 – 57 FSK signals and , 38 – 39 of local optical oscillator , 125 probability

... Modulation Phase noise ASK signals and , 27 - 29 defined , 76 DPSK signals

and , 56 – 57 FSK signals and , 38 – 39 of local optical oscillator , 125 probability

**density**function of , 29 PSK signals and , 48 – 49 variance , 82 See also Noise ...### 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 | |

8 other sections not shown

### 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