Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2003 - Fiber optics |
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Page 3
... described by a nonlinear Helmholtz equation ( NHE ) . Considering a single soliton beam that coincides with the longitudinal axis , off - axis propagation results if only the axis is rotated , whereby is no longer negligible . Moreover ...
... described by a nonlinear Helmholtz equation ( NHE ) . Considering a single soliton beam that coincides with the longitudinal axis , off - axis propagation results if only the axis is rotated , whereby is no longer negligible . Moreover ...
Page 171
... described by the Volterra integral equation . The resolvent operator for this equation is found exactly in the case when the medium properties change in time by jump . This makes the non - linear problem solvable by approximating the ...
... described by the Volterra integral equation . The resolvent operator for this equation is found exactly in the case when the medium properties change in time by jump . This makes the non - linear problem solvable by approximating the ...
Page 210
... described by the Sellmeier's formula ( 2 ) . n = { 1 + Σ ( i = 1,2,3 ) ( 4,22 ) ( 2-1 ) 1/2 . ( 2 ) The method of losses account on the optical waveguide bends , offered in [ 1 ] , was used to define transfer characteristics . 0-7803 ...
... described by the Sellmeier's formula ( 2 ) . n = { 1 + Σ ( i = 1,2,3 ) ( 4,22 ) ( 2-1 ) 1/2 . ( 2 ) The method of losses account on the optical waveguide bends , offered in [ 1 ] , was used to define transfer characteristics . 0-7803 ...
Contents
LFNM Plenary Sessions | 1 |
Extraction of Spectra and Theresholds from FullWave Lasing Eigenvalue Problems Invited | 19 |
Design and Evaluation of High Speed DBR Lasers for Analog and Digital Transmission Invited | 32 |
Copyright | |
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