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 71
The module of the wave vector in the crystal , having the refractive index n , is k =
2 tn / 1 . Hence , the initial phase of the wave is changed due to the changes in
the refractive index in the crystal , and the phase modulation is imposed .
The module of the wave vector in the crystal , having the refractive index n , is k =
2 tn / 1 . Hence , the initial phase of the wave is changed due to the changes in
the refractive index in the crystal , and the phase modulation is imposed .
Page 239
At the same time , the soliton pulsewidth is suppressed by the factor E . The
condition w = $ practically means that the continuous wave must have the same
frequency as the soliton carrier , while the condition = 0 , means that the phases
of the ...
At the same time , the soliton pulsewidth is suppressed by the factor E . The
condition w = $ practically means that the continuous wave must have the same
frequency as the soliton carrier , while the condition = 0 , means that the phases
of the ...
Page 240
20 ) At the same time , the continuous wave is expected to preserve its initial
phase , so there is a possibility for mutual elimination of unused parts of
continuous waves . If the next continuous wave with frequency w = & and phase =
TT + oo is ...
20 ) At the same time , the continuous wave is expected to preserve its initial
phase , so there is a possibility for mutual elimination of unused parts of
continuous waves . If the next continuous wave with frequency w = & and phase =
TT + oo is ...
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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
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Bibliographic information
| Title | Coherent and Nonlinear Lightwave Communications Artech House optoelectronics library Optoelectronics Library |
| Author | Milorad Cvijetic |
| Edition | illustrated |
| Publisher | Artech House, 1996 |
| Original from | the University of Michigan |
| Digitized | 7 Dec 2007 |
| ISBN | 089006590X, 9780890065907 |
| Length | 304 pages |
| Subjects | › Technology & Engineering / Electrical Technology & Engineering / Fiber Optics Technology & Engineering / Optics Technology & Engineering / Telecommunications |
| Export Citation | BiBTeX EndNote RefMan |