Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2003 - Fiber optics |
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Page 26
... shown [ 3 , 7 , 8 , 9 ] . The " dark " state is stationary with its probability equal to 1/2 and does not emit any real photons . This state is presented by a couple of atoms interacting with each other with a virtual photon of the mode ...
... shown [ 3 , 7 , 8 , 9 ] . The " dark " state is stationary with its probability equal to 1/2 and does not emit any real photons . This state is presented by a couple of atoms interacting with each other with a virtual photon of the mode ...
Page 168
... shown in fig . 3 . By applying a 60 mW direct pumping power and an 80 mW reverse power in a 50 km long fiber having 0,2 dB / km attenuation coefficient , there was obtained the power variation of the soliton inside the fiber length ...
... shown in fig . 3 . By applying a 60 mW direct pumping power and an 80 mW reverse power in a 50 km long fiber having 0,2 dB / km attenuation coefficient , there was obtained the power variation of the soliton inside the fiber length ...
Page 232
... shown . c . ' 8 - like ' form waveguide . The results are obtained for waveguides with concave core shape . The 8 - like core form is used : ( 1+ α Cos ( 24 ) ) r ( q ) = a 1+ α ( 1 ) Some variations of the core shape are shown on Fig.3 ...
... shown . c . ' 8 - like ' form waveguide . The results are obtained for waveguides with concave core shape . The 8 - like core form is used : ( 1+ α Cos ( 24 ) ) r ( q ) = a 1+ α ( 1 ) Some variations of the core shape are shown on Fig.3 ...
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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