## 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 176

2-4 . Fig . 2 shows the dependences of the reflection factor of a single narrow slot

( h « < a , h « < b , h = 0,1 sm ) with the variation of

value ( for values & ; = 2,02 , & z = 9,6 ) in the frequency band Af = 0,1 ... 10 GHz .

2-4 . Fig . 2 shows the dependences of the reflection factor of a single narrow slot

( h « < a , h « < b , h = 0,1 sm ) with the variation of

**dielectric**permitivity factor'svalue ( for values & ; = 2,02 , & z = 9,6 ) in the frequency band Af = 0,1 ... 10 GHz .

Page 273

The method of synthesis of planar metal -

proposed . The method is connected with restitution of a law of a refraction index

changes in a cross - section of a lightguide for a given power localization

coefficient of ...

The method of synthesis of planar metal -

**dielectric**lightguides ( MDLG ) isproposed . The method is connected with restitution of a law of a refraction index

changes in a cross - section of a lightguide for a given power localization

coefficient of ...

Page 275

Since 01 ( p ) and o ( p ) are differed with discrete part only Gld COLT = 1 pi M N

Ž B , E , ( 5 , Ę . JE , ( s , ộ ; ) - ŽCE ( 5 , P , DE , ( s , pi ) According to the theory of

the solution of a inverse problem of a dispersion , the change of an

Since 01 ( p ) and o ( p ) are differed with discrete part only Gld COLT = 1 pi M N

Ž B , E , ( 5 , Ę . JE , ( s , ộ ; ) - ŽCE ( 5 , P , DE , ( s , pi ) According to the theory of

the solution of a inverse problem of a dispersion , the change of an

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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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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