Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2005 - Fiber optics |
From inside the book
Results 1-3 of 33
Page 107
... distance between beams Ax = 4x ( a ) , 1.8x , ( b ) , 1.6x , ( c ) , 1.4x ( d ) . 8 = 2 ; k1L = 0.75 ; al01.02 = 0.7 ; z = 40cm . Next , we compare the modes of coherent and incoherent interactions for usual configuration of two - wave ...
... distance between beams Ax = 4x ( a ) , 1.8x , ( b ) , 1.6x , ( c ) , 1.4x ( d ) . 8 = 2 ; k1L = 0.75 ; al01.02 = 0.7 ; z = 40cm . Next , we compare the modes of coherent and incoherent interactions for usual configuration of two - wave ...
Page 169
... distance L which pass each of two modes with different polarization status ( L = 1000 + 10000 m ) with different FO's eccentricity : Aa = 0.01 ; 0.1 ; 0.2 mkm and for different wavelengths λ = 0.85 and 1.3 mkm . Figure 3 shows ...
... distance L which pass each of two modes with different polarization status ( L = 1000 + 10000 m ) with different FO's eccentricity : Aa = 0.01 ; 0.1 ; 0.2 mkm and for different wavelengths λ = 0.85 and 1.3 mkm . Figure 3 shows ...
Page 191
... distance will be small . Using typical values for the parameters appearing in eq . ( 1 ) , e.g. G1 = 12 dBi , G1 = 6 dBi , A = 20 ... 50 dB ( depending on frequency and substrate material ) , and a SNR ≥ 10 dB , a maximum read - out ...
... distance will be small . Using typical values for the parameters appearing in eq . ( 1 ) , e.g. G1 = 12 dBi , G1 = 6 dBi , A = 20 ... 50 dB ( depending on frequency and substrate material ) , and a SNR ≥ 10 dB , a maximum read - out ...
Contents
LFNM Plenary | 1 |
BatteryLess Spatial Optical Communication Terminals for LocationBased Indoor | 14 |
Resonant Photoproduction of the ElectronPositron Pair with Photon Emission | 27 |
Copyright | |
21 other sections not shown
Other editions - View all
Common terms and phrases
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