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 12
... width in the single - mode optical fiber is equal to 2to , which corresponds to the frequency bandwidth ( to ) -1 , it will be doubled after a distance proportional to ( to ) 2 . Practically speaking , that means that the 10 - ps - wide ...
... width in the single - mode optical fiber is equal to 2to , which corresponds to the frequency bandwidth ( to ) -1 , it will be doubled after a distance proportional to ( to ) 2 . Practically speaking , that means that the 10 - ps - wide ...
Page 169
... width of the pump signal is lower than the spectral width of the scattered signal . The spectral width of of the stimulated Raman signal is high enough to consider that ( 6.21 ) and ( 6.38 ) are valid for the laser sources . On the ...
... width of the pump signal is lower than the spectral width of the scattered signal . The spectral width of of the stimulated Raman signal is high enough to consider that ( 6.21 ) and ( 6.38 ) are valid for the laser sources . On the ...
Page 184
... width and 1.6 - W peak power . This conclusion is valid in the absence of loss at the wavelength λ = 1.3 μm . Only ... width equal to 1 ps and the peak power P1 = 3.6 W gives a = 0.5 and a .. = 2. The asymptotical power of the pulse is ...
... width and 1.6 - W peak power . This conclusion is valid in the absence of loss at the wavelength λ = 1.3 μm . Only ... width equal to 1 ps and the peak power P1 = 3.6 W gives a = 0.5 and a .. = 2. The asymptotical power of the pulse is ...
Contents
Optical Transmitters for Coherent Lightwave Systems | 3 |
Coherent Optical Receiver Sensitivity | 15 |
61 | 31 |
Copyright | |
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amplification coefficient amplitude Brillouin scattering channels Chapter characteristics coherent detection coherent lightwave system coherent optical receiver components corresponding detection scheme digit interval dispersion DPSK electric field energy equal equation erbium-doped fiber amplifiers error probability evaluated Figure filter frequency shift Gaussian Hence heterodyne detection homodyne detection IEEE IEEE/OSA incoming optical signal influence input laser amplifiers length Lett lightwave communications lightwave systems Lightwave Techn loss modulating signal multichannel nonlinear effects nonlinear lightwave system optical amplifiers optical oscillator optical power optical transmitter optical-fiber parameters phase modulation phase noise phase shift photodetector photodiode photons polarization propagation PSK signals pump signal R₁ Raman amplification Raman amplifiers ratio realization receiver sensitivity refractive index resonator scattered signal self-phase modulation semiconductor laser signal power single-mode optical fiber soliton pulses soliton regime spectral linewidth spontaneous emission stimulated Raman scattering term thermal noise transmission system variance voltage width