## LFNM 2003: Proceedings of LFNM 2003 : 5th International Workshop on Laser and Fiber-optical Networks Modeling : Alushta, Crimea, Ukraine, 19-20 September 2003 |

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Page 110

The planar SGs with

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

scattering mode , kx = ( 26 / 2 ) sing , 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 ... ß is a propagation constant of the

scattering mode , kx = ( 26 / 2 ) sing , 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 # sing ) where Nte = Btelko is the TEo - mode effective refractive index ...

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 # sing ) where Nte = Btelko is the TEo - mode effective refractive index ...

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 | 7 |

Transformation of the Polarization Distribution in the CrossSection of Light Beam by Self | 18 |

Extraction of Spectra and Theresholds from FullWave Lasing Eigenvalue Problems Invited | 19 |

Copyright | |

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