Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2005 - Fiber optics |
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Page 4
version H ̈1 . Taking into account the layer structure of the VCSEL , the wave equation in the j - th layer can be expressed in a form : d2y d2 11m + 92 dz2 nm 2 +9 jnmnm = 0 , 9mm = knikg , -iknẞ - k , z , < 2 < 2 , +9 jnm ( 4 ) where ...
version H ̈1 . Taking into account the layer structure of the VCSEL , the wave equation in the j - th layer can be expressed in a form : d2y d2 11m + 92 dz2 nm 2 +9 jnmnm = 0 , 9mm = knikg , -iknẞ - k , z , < 2 < 2 , +9 jnm ( 4 ) where ...
Page 6
... layer . 1-111 0.010 0.008- 0.16 - 0.14 0.12- 0.006- 0.10- 0.004 arg ( 1 ) 0 08 0.06- 0.04 0.002- 0.02- 0.000 0.00 -8 -6 -4 -2 0 2 4 6 8 -8 -6 -4 -2 0 2 4 6 8 layer number layer number -1 Fig.2 Eigen - value module vs start position ...
... layer . 1-111 0.010 0.008- 0.16 - 0.14 0.12- 0.006- 0.10- 0.004 arg ( 1 ) 0 08 0.06- 0.04 0.002- 0.02- 0.000 0.00 -8 -6 -4 -2 0 2 4 6 8 -8 -6 -4 -2 0 2 4 6 8 layer number layer number -1 Fig.2 Eigen - value module vs start position ...
Page 275
... layer . The characteristic of photoelectric layer and substrate are known [ 5 ] . The best sensitivity of a photodetector to an interferential field is reached , if the thickness of a photoelectric layer is small and is not aliquot to ...
... layer . The characteristic of photoelectric layer and substrate are known [ 5 ] . The best sensitivity of a photodetector to an interferential field is reached , if the thickness of a photoelectric layer is small and is not aliquot 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