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 148
Optical amplifiers enable a drastic increase in attainable optical distances
because each amplifier compensates signal attenuation caused by the optical
fiber loss in the preceding optical fiber section . At the same time , the
transmission ...
Optical amplifiers enable a drastic increase in attainable optical distances
because each amplifier compensates signal attenuation caused by the optical
fiber loss in the preceding optical fiber section . At the same time , the
transmission ...
Page 258
If the cross - talking due to stimulated Raman scattering is defined as an
attenuation , then the far - end cross - talk attenuation is relevant for unidirectional
transmission , and the near - end cross - talk attenuation is relevant for
bidirectional ...
If the cross - talking due to stimulated Raman scattering is defined as an
attenuation , then the far - end cross - talk attenuation is relevant for unidirectional
transmission , and the near - end cross - talk attenuation is relevant for
bidirectional ...
Page 263
105 ) The attenuation A , can be now determined by [ P : ( 0 P > 0 – P . ( 0 ) | Pro =
0 ] A2 = - 10 log | Pe 4 : = - 10 o [ . CO com P . Orms ] ( 0 . 106 ) ( 9 . 106 ) To find
the attenuation coefficient A1 , we must solve ( 9 . 90b ) for these initial ...
105 ) The attenuation A , can be now determined by [ P : ( 0 P > 0 – P . ( 0 ) | Pro =
0 ] A2 = - 10 log | Pe 4 : = - 10 o [ . CO com P . Orms ] ( 0 . 106 ) ( 9 . 106 ) To find
the attenuation coefficient A1 , we must solve ( 9 . 90b ) for these initial ...
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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
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