Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2005 - Fiber optics |
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Page 4
... 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 is the transverse wave number of n - th harmonic . Omitting indexes n , m the ...
... 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 is the transverse wave number of n - th harmonic . Omitting indexes n , m the ...
Page 72
... equation with a given distribution of dielectric permittivity is suggested . By means of discretization the wave equation was reduced to the system of homogeneous linear equations , for that the eigenvalue problem was worked out . The ...
... equation with a given distribution of dielectric permittivity is suggested . By means of discretization the wave equation was reduced to the system of homogeneous linear equations , for that the eigenvalue problem was worked out . The ...
Page 114
... equation ( CGLE ) . The very similar equation applied to the temporal solitons was solved in [ 3 ] . We can use the space - time analogy and take an advantage of method of special ansac having been used there . We'll in- teresting of ...
... equation ( CGLE ) . The very similar equation applied to the temporal solitons was solved in [ 3 ] . We can use the space - time analogy and take an advantage of method of special ansac having been used there . We'll in- teresting of ...
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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amplitude approximation bandwidth Bragg broadening calculated cavity characteristics circuit coefficient corner reflector corresponding crystal oscillator curves density dependence device dielectric diffraction dispersion distribution e-mail effect electric Electronics emission energy equation error excitation experimental field filter function Gaussian grating IEEE input intensity interaction investigated Keywords Kharkiv Kharkiv National University laser lattice layer Lett light beams linear maximum measurement medium method mode modulation National University noise nonlinear obtained optical fiber optical splitter output parameters phase phase noise photodetector photonic photonic crystal Phys piezoelectric polarization Proc propagation pulse pumping current quantum quartz radiation Raman gain range reflector refractive index region resonator sample scattering semiconductor sensor shown signal simulation solitons solution spectral structure surface temperature thickness transmission Ukraine University of Guanajuato University of Radio VCSEL voltage wave waveguide wavelength width