## 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 187

After the series of segmental

equations are achieved what inter ... equations with variable factors and obvious

pump which after appropriate approach ( approximation ) and

will be ...

After the series of segmental

**transformation**hyperbolical , parabolic , ellipticequations are achieved what inter ... equations with variable factors and obvious

pump which after appropriate approach ( approximation ) and

**transformations**will be ...

Page 291

According to Jones's approach [ 3 ] each segment of thickness AZ acts upon an

incoming field as the

field by the section of twisted fiber of length H , presented as N

According to Jones's approach [ 3 ] each segment of thickness AZ acts upon an

incoming field as the

**transforming**element . ... Consider the**transformation**of thefield by the section of twisted fiber of length H , presented as N

**transforming**...Page 293

Then the

R - ' ( 6 ) lim 1+ ( 12 ) 1.JJ where y , = 25 ,. We have also divided the whole

section onto N segments . Obviously that iY2 - ih 0 2л C explaisa , or Δλ , exp H

211 ...

Then the

**transformation**matrix T , assumes the form : N 0 iyi 0 1 > N - 70 N Ø To aR - ' ( 6 ) lim 1+ ( 12 ) 1.JJ where y , = 25 ,. We have also divided the whole

section onto N segments . Obviously that iY2 - ih 0 2л C explaisa , or Δλ , exp H

211 ...

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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