## Proceedings of LFNM'...: International Workshop on Laser and Fiber-optical Networks Modeling, Volume 6Institution of Electrical and Electronics Engineers, 2004 - Fiber optics |

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Page 47

The problem becomes more complex if the far field distribution isn ' t bounded by

a half space and we have counter propagating power transfer at the waist when

the normal to the waist plane component of the Poynting

The problem becomes more complex if the far field distribution isn ' t bounded by

a half space and we have counter propagating power transfer at the waist when

the normal to the waist plane component of the Poynting

**vector**can be negative .Page 156

For ID photonic crystal the determination of the wave

whether the frequency is allowed , can be brought to the solution of eigenvalue

problem : THG ( 0 ) ) . ( 1 ) VGO ) ( GO ) ) Ta f ( 0 ) = expljk ; a \ FO ) = P ( FO ) ) If

the ...

For ID photonic crystal the determination of the wave

**vector**k , and showing upwhether the frequency is allowed , can be brought to the solution of eigenvalue

problem : THG ( 0 ) ) . ( 1 ) VGO ) ( GO ) ) Ta f ( 0 ) = expljk ; a \ FO ) = P ( FO ) ) If

the ...

Page 183

( x , y , z ) " Q = Kr , K = K , + Kı - the grating

amplitudes , K ; - the wave

beams , respectively . We present the solution in the view of spatial - temporal ...

( x , y , z ) " Q = Kr , K = K , + Kı - the grating

**vector**, r - the radius -**vector**, A ; – theamplitudes , K ; - the wave

**vectors**and e ; – the polarization**vector**of recordingbeams , respectively . We present the solution in the view of spatial - temporal ...

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### Contents

L Lasers and Resonators | 11 |

Optically coupled lasers Invited | 11 |

Mathematical models applied to optical and thermal diagnostic of semiconductor | 17 |

Copyright | |

13 other sections not shown

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