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 40
Page 11
... pulse width , and the optical - fiber dispersion characteristics at the carrier wave- length . The proper time distance between the neighboring soliton pulses must be chosen during their generation process in an optical source , to ...
... pulse width , and the optical - fiber dispersion characteristics at the carrier wave- length . The proper time distance between the neighboring soliton pulses must be chosen during their generation process in an optical source , to ...
Page 237
Milorad Cvijetic. 9.2.2 Soliton Regeneration on the Optical Fiber Link Regeneration of soliton pulses on the optical ... pulse spreading is compensated . At the same time , the solitons ' amplitude increases , since the area under the soliton ...
Milorad Cvijetic. 9.2.2 Soliton Regeneration on the Optical Fiber Link Regeneration of soliton pulses on the optical ... pulse spreading is compensated . At the same time , the solitons ' amplitude increases , since the area under the soliton ...
Page 242
... soliton formed from this amplified pulse has the stationary amplitude B given by [ 6 ] B = ( 2b − 1 ) n - ( 9.25 ) Then , if b = A + 1 , it will be B = ( 1 + 2A ) ŋ ; hence , the stationary soliton , created from the amplified soliton ...
... soliton formed from this amplified pulse has the stationary amplitude B given by [ 6 ] B = ( 2b − 1 ) n - ( 9.25 ) Then , if b = A + 1 , it will be B = ( 1 + 2A ) ŋ ; hence , the stationary soliton , created from the amplified soliton ...
Contents
Coherent Optical Receiver Sensitivity | 15 |
7 | 37 |
References | 60 |
Copyright | |
10 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 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