Proceedings of LFNM'...: International Workshop on Laser and Fiber-optical Networks Modeling, Volume 5Kharkiv State University of Radio Electronics, 2003 - Fiber optics |
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Page 224
... defined by the same small nondimensional parameter ẞ [ 4 ] . Simultaneously with longitudinal coordinate z we introduce " smooth " scale = Bz . We suppose that wavenumber of incident plane waves lies in yz - plane so that for field ...
... defined by the same small nondimensional parameter ẞ [ 4 ] . Simultaneously with longitudinal coordinate z we introduce " smooth " scale = Bz . We suppose that wavenumber of incident plane waves lies in yz - plane so that for field ...
Page 246
... defined as the ratio of the mean square intensity fluctuations to the mean intensity squared of the laser output . The RIN relates the noise of the optical power dS ( t ) to < S > and it is defined as RIN = < & S2 ( t ) > _ < S ( t ) 2 > ...
... defined as the ratio of the mean square intensity fluctuations to the mean intensity squared of the laser output . The RIN relates the noise of the optical power dS ( t ) to < S > and it is defined as RIN = < & S2 ( t ) > _ < S ( t ) 2 > ...
Page 262
... definition in dependence on wavelength , while that time on practice an average and mean square differential group delay ... defined as follows : I - anoptical signal the whole time average power , the sum of polarized and non- polarized ...
... definition in dependence on wavelength , while that time on practice an average and mean square differential group delay ... defined as follows : I - anoptical signal the whole time average power , the sum of polarized and non- polarized ...
Contents
LFNM Plenary Sessions | 1 |
Extraction of Spectra and Theresholds from FullWave Lasing Eigenvalue Problems Invited | 19 |
Design and Evaluation of High Speed DBR Lasers for Analog and Digital Transmission Invited | 32 |
Copyright | |
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