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 81
Page 106
8 ) The thermal noise power on the resistance , Rį , is given by the known relation
ix ( + ) = 44® ( 4 . 9 ) RL where k is Boltzmann ' s constant and ® is the absolute
temperature . The mean square value of the amplifier output voltage due to ...
8 ) The thermal noise power on the resistance , Rį , is given by the known relation
ix ( + ) = 44® ( 4 . 9 ) RL where k is Boltzmann ' s constant and ® is the absolute
temperature . The mean square value of the amplifier output voltage due to ...
Page 122
82 ) where S ( f ) corresponds to the power spectral density , 0 ( s ) , given by ( 4 .
54 ) . At the same time , the power spectrum , 0 , ( s ) , in ( 4 . 54 ) corresponds to
the FM spectrum of the IF signal . All that is valid for detection of ASK , FSK , and ...
82 ) where S ( f ) corresponds to the power spectral density , 0 ( s ) , given by ( 4 .
54 ) . At the same time , the power spectrum , 0 , ( s ) , in ( 4 . 54 ) corresponds to
the FM spectrum of the IF signal . All that is valid for detection of ASK , FSK , and ...
Page 244
29 ) will be bright solitons in the anomalous dispersion region if the Raman
amplification coefficient , given by the term al , is exactly canceled by the loss
coefficient T . The bright soliton solution has the form q = qo sech ( 907 ) exp ( jqõ
£ / 2 ) ...
29 ) will be bright solitons in the anomalous dispersion region if the Raman
amplification coefficient , given by the term al , is exactly canceled by the loss
coefficient T . The bright soliton solution has the form q = qo sech ( 907 ) exp ( jqõ
£ / 2 ) ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
Preface | 5 |
Coherent Optical Receiver Sensitivity | 15 |
Optical Transmitters for Coherent Lightwave Systems | 61 |
Copyright | |
8 other sections not shown
Other editions - View all
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