Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2005 - Fiber optics |
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Page 208
... function of the previous ones during the tree parsing . Here , The construction of the tree is based on the addition formulae of exponential . As an example , the binary tree for exponential function is shown in Fig . ( 4 ) . Of course ...
... function of the previous ones during the tree parsing . Here , The construction of the tree is based on the addition formulae of exponential . As an example , the binary tree for exponential function is shown in Fig . ( 4 ) . Of course ...
Page 231
FINITENESS THEOREM The shape of AOTF - spectrometer instrument function is mainly determined by the AOTF transmission window , and has following form h ( way ) = | E1 ( L , x ) 2 / Eo2 . To find the FT instrument function , let's ...
FINITENESS THEOREM The shape of AOTF - spectrometer instrument function is mainly determined by the AOTF transmission window , and has following form h ( way ) = | E1 ( L , x ) 2 / Eo2 . To find the FT instrument function , let's ...
Page 264
... function gr ( @ ) which will be most close to experimental Raman gain profile . Because best fitting is main our purpose of decomposition procedure , in present work we used computer nonlinear fitting with the Levenberg Marquardt method ...
... function gr ( @ ) which will be most close to experimental Raman gain profile . Because best fitting is main our purpose of decomposition procedure , in present work we used computer nonlinear fitting with the Levenberg Marquardt method ...
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