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 143
These 2 , 000 channels with bit rates of 1 Gb / s per channel will occupy the
wavelength region of only 300 nm . It means that single mode optical fibers
provide the transmission of more than 2 , 000 optical channels in the minimum -
loss region ...
These 2 , 000 channels with bit rates of 1 Gb / s per channel will occupy the
wavelength region of only 300 nm . It means that single mode optical fibers
provide the transmission of more than 2 , 000 optical channels in the minimum -
loss region ...
Page 223
The noise level in the experimental realization is in the theoretically predicted
region [ 20 ] . Although we discuss only Raman amplifiers , it should be noted that
Brillouin amplifiers also can be efficiently applied in certain circumstances for ...
The noise level in the experimental realization is in the theoretically predicted
region [ 20 ] . Although we discuss only Raman amplifiers , it should be noted that
Brillouin amplifiers also can be efficiently applied in certain circumstances for ...
Page 268
A transmission peak of the filter can be tuned through one spectral region Af by
piezoelectrically tuning length L through one optical half - wavelength . The
tuning range depends on the filter length , according to ( 9 . 99 ) . For a tuning
range of ...
A transmission peak of the filter can be tuned through one spectral region Af by
piezoelectrically tuning length L through one optical half - wavelength . The
tuning range depends on the filter length , according to ( 9 . 99 ) . For a tuning
range of ...
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Contents
Preface | 5 |
Coherent Optical Receiver Sensitivity | 15 |
Optical Transmitters for Coherent Lightwave Systems | 61 |
Copyright | |
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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