Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2005 - Fiber optics |
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Page 103
... intensities . In the unpumped case and at small pump intensity ( 0.34 kW / cm2 ) the available holding beam intensities do not reach the transparency point of the semiconductor material . At high pump intensities ( 10.4 - 15.4 kW / cm2 ) ...
... intensities . In the unpumped case and at small pump intensity ( 0.34 kW / cm2 ) the available holding beam intensities do not reach the transparency point of the semiconductor material . At high pump intensities ( 10.4 - 15.4 kW / cm2 ) ...
Page 104
holding beam intensity , KW cm 15 10 Dark Soliton holding beam intensity , kW / cm2 9 Bright Soliton 0 2 4 6 8 10 12 pump intensity , KW / cm2 ( a ) 2 4 6 pump intensity , kW / cm2 ( b ) Fig . 3 ( a ) Measured switch - on intensity for ...
holding beam intensity , KW cm 15 10 Dark Soliton holding beam intensity , kW / cm2 9 Bright Soliton 0 2 4 6 8 10 12 pump intensity , KW / cm2 ( a ) 2 4 6 pump intensity , kW / cm2 ( b ) Fig . 3 ( a ) Measured switch - on intensity for ...
Page 126
bg where is the background intensity for every couple of beams marked by " + " or “ - “ I + - depending on the sign of angle 0 , A is the intensity pattern period , z and x are the transverse coordinates adjusted along and normally to ...
bg where is the background intensity for every couple of beams marked by " + " or “ - “ I + - depending on the sign of angle 0 , A is the intensity pattern period , z and x are the transverse coordinates adjusted along and normally to ...
Contents
LFNM Plenary | 1 |
BatteryLess Spatial Optical Communication Terminals for LocationBased Indoor | 14 |
Resonant Photoproduction of the ElectronPositron Pair with Photon Emission | 27 |
Copyright | |
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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