Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2005 - Fiber optics |
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Page 147
... distribution of the pumping system one can use Finite Difference Method , FDM . Recently Boundary Integral Method , BIM , is used to calculate such distribution in the end pumped systems [ 1 ] . The advantage of BIM over FDM is its ...
... distribution of the pumping system one can use Finite Difference Method , FDM . Recently Boundary Integral Method , BIM , is used to calculate such distribution in the end pumped systems [ 1 ] . The advantage of BIM over FDM is its ...
Page 289
... distribution of is negative exponential and that of the effective broadening is Rayleigh , as shown in Fig . 3. But , for the larger values of average PMD , the distribution of 7 is Gamma and that of Ateff is Maxwellian , as illustrated ...
... distribution of is negative exponential and that of the effective broadening is Rayleigh , as shown in Fig . 3. But , for the larger values of average PMD , the distribution of 7 is Gamma and that of Ateff is Maxwellian , as illustrated ...
Page 290
... distribution of the output RMS pulse width and the fitted curve ( 70.7-27 e ) ( b ) distribution of the effective broadening and the fitted Maxwellian curve . Distributions for Gaussian and super - Gaussian pulse shapes are the same . 4 ...
... distribution of the output RMS pulse width and the fitted curve ( 70.7-27 e ) ( b ) distribution of the effective broadening and the fitted Maxwellian curve . Distributions for Gaussian and super - Gaussian pulse shapes are the same . 4 ...
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