## Proceedings of LFNM'...: International Workshop on Laser and Fiber-optical Networks Modeling, Volume 6Kharkiv State University of Radio Electronics, 2004 - Fiber optics |

### From inside the book

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Page 47

The power density to characterize the beam is the component of the averaged

Poynting

complex if the far field distribution isn't bounded by a half space and we have ...

The power density to characterize the beam is the component of the averaged

Poynting

**vector**in the direction of propagation [ 10 ] . The problem becomes morecomplex if the far field distribution isn't bounded by a half space and we have ...

Page 183

... K = Ko + Kı- the grating

the wave

respectively . We present the solution in the view of spatial - temporal distribution

of the first ...

... K = Ko + Kı- the grating

**vector**, r- the radius -**vector**, A ; – the amplitudes , K ; -the wave

**vectors**and e ; - the polarization**vector**of recording beams ,respectively . We present the solution in the view of spatial - temporal distribution

of the first ...

Page 275

... 1/4 are the frequency and the absolute value of the wave

wave , respectively ; e , is the unit

laser pulse duration . We assume that the characteristic oscillation time ( -w ' ) is ...

... 1/4 are the frequency and the absolute value of the wave

**vector**of the laserwave , respectively ; e , is the unit

**vector**directed along the X axis and to - is thelaser pulse duration . We assume that the characteristic oscillation time ( -w ' ) is ...

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### Contents

L Lasers and Resonators | 1 |

Compact electricdischarge excimer lasers invited | 14 |

Simplified model for XECLlasers | 29 |

Copyright | |

14 other sections not shown

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### Common terms and phrases

absorption active allows amplitude analysis angle aperture application approximation band beam calculated characteristics coefficient coherent components considered constant corresponds crystal defined density dependence described determined developed devices diffraction direction distance distribution e-mail effect efficiency electric electron elements emission energy equal equation excitation experimental expression fiber fibre field Figure frequency function given grating IEEE increase initial intensity interference Kharkiv laser layer length light losses material means measured medium method mirror mode modulation nonlinear observed obtained operation optical oscillators output parameters phase photon Physics plane polarization possible presented problem processes propagation properties pulse quantum radiation range received REFERENCES reflection refraction region relative resonator sample scattering shown shows signal solution spectral spectrum stability structure surface temperature Ukraine University wave waveguide wavelength