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 56
... resonator . Function y ( x ) = 1 + q ( x ) describes the dependence of losses of the resonator on radiating power , constants a and b are the control parameters . - a a - - The objectives of the work are to determine the conditions of ...
... resonator . Function y ( x ) = 1 + q ( x ) describes the dependence of losses of the resonator on radiating power , constants a and b are the control parameters . - a a - - The objectives of the work are to determine the conditions of ...
Page 87
... resonator ; / - the length of an active part ; l'- the length of a passive part ; d – the summary losses in the resonator ; n0 ' = nl ' + n2'- the density of particles at the appropriate - 0-7803-7709-5 / 03 / $ 17.00 © 2003 IEEE energy ...
... resonator ; / - the length of an active part ; l'- the length of a passive part ; d – the summary losses in the resonator ; n0 ' = nl ' + n2'- the density of particles at the appropriate - 0-7803-7709-5 / 03 / $ 17.00 © 2003 IEEE energy ...
Page 133
... resonator . Bragg structures used as resonator reflector [ 3 ] have flexible frequency characteristics so that they can be useful for devices operating on some frequencies simultaneously . If the Bragg structure has high reflectivity on ...
... resonator . Bragg structures used as resonator reflector [ 3 ] have flexible frequency characteristics so that they can be useful for devices operating on some frequencies simultaneously . If the Bragg structure has high reflectivity on ...
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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