## 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 130

As opposed to ( 1 ) where the amplitudes of the

comparable , the amplitude of the second term here is significantly smaller than

the amplitude of the

...

As opposed to ( 1 ) where the amplitudes of the

**first**and the second terms arecomparable , the amplitude of the second term here is significantly smaller than

the amplitude of the

**first**term because \ Ecl << Eel and \ Ezal << \ Es / . Therefore...

Page 216

... functions of the

may obtain the a - and ß dependence on 2 from Eq . ( 5 ) of our model . To solve

the problem we may use the

considering ...

... functions of the

**first**kind and modificated Bessel functions respectively . Wemay obtain the a - and ß dependence on 2 from Eq . ( 5 ) of our model . To solve

the problem we may use the

**first**approximation of perturbation theoryconsidering ...

Page 237

Utilizing the “ exact ” model , steady state values for electron No and photon So

numbers are calculated together with the steady state gain Go = G ( neoonpo )

and

Utilizing the “ exact ” model , steady state values for electron No and photon So

numbers are calculated together with the steady state gain Go = G ( neoonpo )

and

**first**order partial derivatives Δη The parameters of three common р ...### 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 | |

21 other sections not shown

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