Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2003 - Fiber optics |
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Page 20
... algorithm . The eigenvalues were found by solving the proper Schroedinger equation in the interaction picture ( with г = 0 for the ideal cavity ) . The theory uses the known Green functions formalism in the Heitler - Ma form [ 4 ] ...
... algorithm . The eigenvalues were found by solving the proper Schroedinger equation in the interaction picture ( with г = 0 for the ideal cavity ) . The theory uses the known Green functions formalism in the Heitler - Ma form [ 4 ] ...
Page 21
... algorithm . int The adopted form of interaction Hamiltonian conserves a total number of excitation in the system , and the Stark - subsystem's states are degenerate in the absence of interaction H sk So the system " atom + one resonant ...
... algorithm . int The adopted form of interaction Hamiltonian conserves a total number of excitation in the system , and the Stark - subsystem's states are degenerate in the absence of interaction H sk So the system " atom + one resonant ...
Page 173
... algorithm for calculations uses the formula ( 1 ) , ( 2 ) , and ( 5 ) , explicit expressions for which are obtained in [ 2 ] . Fig . 2 shows calculated the time behaviour of the nonlinearity permittivity h1 = √ɛ / ε and of the field ...
... algorithm for calculations uses the formula ( 1 ) , ( 2 ) , and ( 5 ) , explicit expressions for which are obtained in [ 2 ] . Fig . 2 shows calculated the time behaviour of the nonlinearity permittivity h1 = √ɛ / ε and of the field ...
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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