## Proceedings of LFNM'...: International Workshop on Laser and Fiber-optical Networks Modeling, Volume 4Kharkiv State University of Radio Electronics, 2002 - Fiber optics |

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Page 114

Reflection from the bottom Bragg reflector is computed by the following

procedure : Co = F ( V. ) , Do = -ta Coltza Vi * = F ( D. ) . To complete the round -

trip

phase screen P ...

Reflection from the bottom Bragg reflector is computed by the following

procedure : Co = F ( V. ) , Do = -ta Coltza Vi * = F ( D. ) . To complete the round -

trip

**operator**P it is necessary to calculate transmission through through thephase screen P ...

Page 117

... 2 L M The linear

total envelope A is a sum of M channel envelopes 4 ( T , z ) , which are

associated ...

... 2 L M The linear

**operator**L describes loss and dispersion , and the nonlinear**operator**r stands for self - phase modulation . In the case of a WDM system , thetotal envelope A is a sum of M channel envelopes 4 ( T , z ) , which are

associated ...

Page 174

Index Terms - Wave diffraction , periodical structure , axial symmetry , axial slot ,

scattering

coaxial waveguides with slots are sufficiently often used in ultra high ...

Index Terms - Wave diffraction , periodical structure , axial symmetry , axial slot ,

scattering

**operator**. Introduction The different types of antenna systems based oncoaxial waveguides with slots are sufficiently often used in ultra high ...

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### Contents

INV L1 NEW CONCEPT OF MULTIPASS RESONATORS FOR GAS AND | 1 |

L2 WIDEAPERTURE ELECTRODISCHARGE EXCIMER LASERS | 8 |

L4 POSSIBILITY OF HIGHFREQUENCY PULSE DISCHARGE | 17 |

Copyright | |

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### Common terms and phrases

absorption active allows amplitude angle applied axis beam calculated carried characteristics charge coefficient components considered constant corresponds crystals defined density dependence described determined devices diffraction direction discharge distribution effective electric electrons elements energy equal equation experimental expression factor fiber field frequency function gain given gratings IEEE increase intensity interaction Kharkov laser layer length light linear means measured medium method mirror mode modulation necessary nonlinear observed obtained operator optical output parameters particles periodic phase photonic physical plane polarization positive possible presented problem processes propagation properties pulse pumping quantum radiation range received References reflection refractive resonator scattering shown shows signal solution space spatial spectral structure surface temperature tion transformation Ukraine University vector volume vortex wave waveguide wavelength