## 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 39

The optical field satisfies the scalar wave

U = 0 , ( 1 ) ox2 Oz ? in an assumption that the polarization effects can be

neglected . Here k , is the reference wave number , n is index and g is gain ,

which may ...

The optical field satisfies the scalar wave

**equation**220 d ́U OPU + ( kžn – ik , g )U = 0 , ( 1 ) ox2 Oz ? in an assumption that the polarization effects can be

neglected . Here k , is the reference wave number , n is index and g is gain ,

which may ...

Page 69

In the optical part of the model we solve 3D wave

help of the effective frequency method ... The basic idea of this method is to

separate scalar wave

In the optical part of the model we solve 3D wave

**equation**in laser cavity withhelp of the effective frequency method ... The basic idea of this method is to

separate scalar wave

**equation**into 1D vertical and 2D in - plane ( radial )**equations**.Page 203

It means , that the profile of the WM Es ( x ) and the module of a vector ks , and

also a polarization e and a wave vectors of plane waves in spectrum E ( 0 ) of the

RM will be satisfied the appropriate wave

It means , that the profile of the WM Es ( x ) and the module of a vector ks , and

also a polarization e and a wave vectors of plane waves in spectrum E ( 0 ) of the

RM will be satisfied the appropriate wave

**equations**of the non shocking ...### What people are saying - Write a review

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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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