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 26
+ resonance mode ” -a.c.Stark subsystem . The proper solution of the wave
equation in the case r = 0 , found without linear approximation in g , - the constant
but again in one - particle approximation , shows a periodical exchange with
energy ...
+ resonance mode ” -a.c.Stark subsystem . The proper solution of the wave
equation in the case r = 0 , found without linear approximation in g , - the constant
but again in one - particle approximation , shows a periodical exchange with
energy ...
Page 57
... the classical case ( 8 = 1 ) . The analysis of the found periodical solution of the
system ( 1 ) is made in linear approximation by the low functional parameter &
that allows the representation of the found solution in the following form : { x - x .
... the classical case ( 8 = 1 ) . The analysis of the found periodical solution of the
system ( 1 ) is made in linear approximation by the low functional parameter &
that allows the representation of the found solution in the following form : { x - x .
Page 216
... and modificated Bessel functions respectively . We may obtain the a - and ß
dependence on 2 from Eq . ( 5 ) of our model . To solve the problem we may use
the first approximation of perturbation theory considering the small contribution of
...
... and modificated Bessel functions respectively . We may obtain the a - and ß
dependence on 2 from Eq . ( 5 ) of our model . To solve the problem we may use
the first approximation of perturbation theory considering the small contribution of
...
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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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