Proceedings of LFNM'...: International Workshop on Laser and Fiber-optical Networks Modeling, Volume 5Institution of Electrical and Electronics Engineers, 2003 - Fiber optics |
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Page 40
T ( 6 ) 121 122 The coefficients of input and output plane waves at the set of 1
layers are bounded by the relation of the ... +1 ( 9,41 = Metal ( Ti ) Contact Air n =
1 14 wave GaAs n = 3.52 14 wave AIAs n = 2.95 Cap layer 20.5 pairs ( p - type ) ...
T ( 6 ) 121 122 The coefficients of input and output plane waves at the set of 1
layers are bounded by the relation of the ... +1 ( 9,41 = Metal ( Ti ) Contact Air n =
1 14 wave GaAs n = 3.52 14 wave AIAs n = 2.95 Cap layer 20.5 pairs ( p - type ) ...
Page 113
In this case the transition process of forming of the diffractive wave Ei ( r , t ) , and
also enrichment of the spectral structure of the field Ei ( r , t ) influence on the
spread function ( SP ) Y ( t , 02 ) [ 5 ] . Enrichment of the spectral structure of the
field ...
In this case the transition process of forming of the diffractive wave Ei ( r , t ) , and
also enrichment of the spectral structure of the field Ei ( r , t ) influence on the
spread function ( SP ) Y ( t , 02 ) [ 5 ] . Enrichment of the spectral structure of the
field ...
Page 222
In the non - uniform sample the propagation of an acoustic wave was calculated .
The procedure of the measurement of velocity of an acoustic wave was simulated
too . We accept that the whole absorbed light energy is transformed into heat .
In the non - uniform sample the propagation of an acoustic wave was calculated .
The procedure of the measurement of velocity of an acoustic wave was simulated
too . We accept that the whole absorbed light energy is transformed into heat .
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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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