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 40
... takes the values ( 0 , π / 2 , −π / 2 , π ) , ( 2.89 ) becomes Pn - S4PSK ( t ) = cos w。tΣah , ( t - nT1 ) cos n + sin wotΣb „ h , ( t − nТ¿ ) sin -00 ( 2.92 ) The elements a , and b , of the information content take the values a , e ...
... takes the values ( 0 , π / 2 , −π / 2 , π ) , ( 2.89 ) becomes Pn - S4PSK ( t ) = cos w。tΣah , ( t - nT1 ) cos n + sin wotΣb „ h , ( t − nТ¿ ) sin -00 ( 2.92 ) The elements a , and b , of the information content take the values a , e ...
Page 64
... takes the form W = ΣΣΕΕ Ekm EkEm k , m = x , y , z m ( 3.5 ) In general , the tensor of dielectric permittivity has six independent components , because Єkm = Єmk [ 1 ] , so the density of the electrical energy can be written as 2w ...
... takes the form W = ΣΣΕΕ Ekm EkEm k , m = x , y , z m ( 3.5 ) In general , the tensor of dielectric permittivity has six independent components , because Єkm = Єmk [ 1 ] , so the density of the electrical energy can be written as 2w ...
Page 184
... takes the initial shape . 7.2.1 Influence of Third - Order Dispersion and Loss on Soliton Behavior To find the solution of inhomogeneous ( 7.4 ) , we can apply the perturbation method [ 1 , 3 ] . The effects of the third - order ...
... takes the initial shape . 7.2.1 Influence of Third - Order Dispersion and Loss on Soliton Behavior To find the solution of inhomogeneous ( 7.4 ) , we can apply the perturbation method [ 1 , 3 ] . The effects of the third - order ...
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amplification coefficient amplitude applied binary Brillouin scattering channels Chapter characteristics coherent detection coherent lightwave system coherent optical receiver components corresponding crystal DCPSK digit interval dispersion DPSK electric field electro-optical ellipsoid energy equal equation erbium-doped fiber amplifiers error probability evaluated expressed Figure filter frequency bandwidth Gaussian Hence homodyne detection IEEE IEEE/OSA IM/DD incoming optical signal influence input laser amplifiers length Lett lightwave systems Lightwave Techn loss modulating signal modulation methods nonlinear effects nonlinear lightwave system obtained optical amplifiers Optical Commun optical oscillator optical power optical receiver optical transmitter optical-fiber parameters phase difference phase modulation phase noise phase shift photodetector photodiode photons polarization propagation PSK signals pump signal Raman amplification Raman amplifiers random ratio realization receiver sensitivity refractive index resonator semiconductor laser signal power single-mode optical fiber soliton pulse soliton regime spontaneous emission thermal noise transmission system variance voltage wavelength