Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2003 - Fiber optics |
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Page 41
... losses 8-1 - yl . The operating mode has zero losses : 8 = 0 , y = 1 . The non - hermitian high - dimensional operator P forces us to use Krylov's subspace methods for calculating the higher - order modes . We select Arnoldi algorithm ...
... losses 8-1 - yl . The operating mode has zero losses : 8 = 0 , y = 1 . The non - hermitian high - dimensional operator P forces us to use Krylov's subspace methods for calculating the higher - order modes . We select Arnoldi algorithm ...
Page 194
... loss . The fields of the HFS with effective index difference guidance mechanism ( Fig . 2b ) spread to the fibre ... losses strongly depend on the HFs dimension ( number of HF lattice periods ) , air hole diameter and hole separation ...
... loss . The fields of the HFS with effective index difference guidance mechanism ( Fig . 2b ) spread to the fibre ... losses strongly depend on the HFs dimension ( number of HF lattice periods ) , air hole diameter and hole separation ...
Page 210
... losses in the cover , and the signal level on the optical fiber output decreases . The infringement of total reflection conditions at optical fiber stationary mode is possible subject to change of optical signal wavelength 2. It is ...
... losses in the cover , and the signal level on the optical fiber output decreases . The infringement of total reflection conditions at optical fiber stationary mode is possible subject to change of optical signal wavelength 2. It is ...
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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