## 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 110

The planar SGs with

scattered TE- and TM - modes for small ... where ß is a propagation constant of

the scattering mode , kx ( 27/1 ) sino , a = 2 ( B , y ) , i , j are Cartesian unit

.

The planar SGs with

**vector**K ( K lies in the plane of the sample ) grow due to thescattered TE- and TM - modes for small ... where ß is a propagation constant of

the scattering mode , kx ( 27/1 ) sino , a = 2 ( B , y ) , i , j are Cartesian unit

**vectors**.

Page 199

It is known [ 7 ] that the dominating gratings with s - polarization of inducing beam

are the so - called S_- and S + -gratings with

nte sino ) where nte = BTelko is the TEo - mode effective refractive index , Bte ...

It is known [ 7 ] that the dominating gratings with s - polarization of inducing beam

are the so - called S_- and S + -gratings with

**vectors**KIE , and periods ds + = 1 / (nte sino ) where nte = BTelko is the TEo - mode effective refractive index , Bte ...

Page 263

If the beam is completely nonpolarized , then M = C = S = 0 , and if it is completely

polarized , then ( M2 + C2 + S2 ) 1 / 2 = I . Jones '

solution , in which phase correlation between the beams is necessary to take ...

If the beam is completely nonpolarized , then M = C = S = 0 , and if it is completely

polarized , then ( M2 + C2 + S2 ) 1 / 2 = I . Jones '

**vector**is suitable for those tasksolution , in which phase correlation between the beams is necessary to take ...

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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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