Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2005 - Fiber optics |
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Page 123
... lattices . The next approaches may be used to observe gap solitons . First , light beam is excited within the lattice along the Bragg direction ( Fig . 2a ) [ 6 ] . Second , two light beams are excited within the lattice in the Bragg ...
... lattices . The next approaches may be used to observe gap solitons . First , light beam is excited within the lattice along the Bragg direction ( Fig . 2a ) [ 6 ] . Second , two light beams are excited within the lattice in the Bragg ...
Page 124
... lattice defect induced by the readout light field which is a consequence of the beam divergence within the waveguide plane . Second , a possible distinction of a light beam power from its level necessary to form stable gap solitons can ...
... lattice defect induced by the readout light field which is a consequence of the beam divergence within the waveguide plane . Second , a possible distinction of a light beam power from its level necessary to form stable gap solitons can ...
Page 126
... lattices is sketched in Fig . 1. Here collimated extraordinarily polarized light beam of He - Ne laser is focused onto the entrance facet of the lattice with spherical lens ( MO ) . The focal length of this lens changes from 20 to 200 ...
... lattices is sketched in Fig . 1. Here collimated extraordinarily polarized light beam of He - Ne laser is focused onto the entrance facet of the lattice with spherical lens ( MO ) . The focal length of this lens changes from 20 to 200 ...
Contents
LFNM Plenary | 1 |
BatteryLess Spatial Optical Communication Terminals for LocationBased Indoor | 14 |
Resonant Photoproduction of the ElectronPositron Pair with Photon Emission | 27 |
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active allows amplitude analysis application approximation band beam boundary calculated carrier cavity characteristics circuit coefficient considered corresponding coupled crystal curves dependence described determined device diffraction direction distribution e-mail effect efficiency electric Electronics elements energy equation error excitation experimental fiber field filter frequency function gain given grating IEEE increasing input intensity interval laser lattice layer length light limited losses maximum measurement medium method mirror mode modulation noise nonlinear observed obtained operation optical oscillator output parameters periodic phase photonic polarization possible presented problem propagation pulse pumping quantum radiation range REFERENCES reflection refractive index region resonator sample scattering semiconductor sensor shift shown shows signal simulation solitons solution spatial spectral spectrum structure surface temperature thickness transmission Ukraine University University of Guanajuato wave waveguide wavelength width