## 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 40

T ( 6 ) 121 122 The coefficients of input and output plane

layers are bounded by the relation of the ... +1 ( 9,41 = Metal ( Ti ) Contact Air n =

1 14

T ( 6 ) 121 122 The coefficients of input and output plane

**waves**at the set of 1layers 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

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 ) , andalso 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

The procedure of the measurement of velocity of an acoustic

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 simulatedtoo . 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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active allows amplitude analysis angle application approximation beam calculated carrier cavity characteristics coefficient complex components computational considered constant corresponding coupling crystal decrease dependence described determined device dielectric diffraction direction dispersion distance distribution dynamics e-mail effective electric Electronics energy equation erbium fiber field Figure frequency function gain grating harmonic IEEE incident increase influence initial intensity interaction laser layer length light losses material measurements medium method mode modulation nonlinear normal numerical observed obtained operation optical output parameters periodic phase photonic photonic crystal Physics plane polarization possible presented problem propagation properties pulse pumping quantum radiation radius range REFERENCES reflection refractive index region resonance scattering shown shows signal simulation soliton solution spatial structure temperature thickness threshold transmission transverse Ukraine University VCSEL vector wave waveguide wavelength