Proceedings of LFNM'...: International Workshop on Laser and Fiber-optical Networks Modeling, Volume 6Institution of Electrical and Electronics Engineers, 2004 - Fiber optics |
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Page 21
... Gain and index at the active layer are approximated by the formulas + S R 2k g = gon ln ( ( Y ) ) , q ( Y ) = · a + ( 1 - α ) Y - a ) , Y < l Y , Y≥1 2 n = n ′′ g + BT , no = is an index for the conditions of where a e10.368 , gov is a ...
... Gain and index at the active layer are approximated by the formulas + S R 2k g = gon ln ( ( Y ) ) , q ( Y ) = · a + ( 1 - α ) Y - a ) , Y < l Y , Y≥1 2 n = n ′′ g + BT , no = is an index for the conditions of where a e10.368 , gov is a ...
Page 108
... gain and spontaneous radiative recombination spectra of the lasers [ 3 ] . The gain coefficient k ( v ) in the QW of the width d ; ( i = 1 , 2 ) at the light frequency v and a definite TE- or TM - polarization is determined taking into ...
... gain and spontaneous radiative recombination spectra of the lasers [ 3 ] . The gain coefficient k ( v ) in the QW of the width d ; ( i = 1 , 2 ) at the light frequency v and a definite TE- or TM - polarization is determined taking into ...
Page 331
... gain as a function of incident intensity . We have observed gain up to 200 % for isolated dark solitons . We find that the gain is generally higher for a dark soliton located near the switching front ( Fig3a ) than for a dark soliton in ...
... gain as a function of incident intensity . We have observed gain up to 200 % for isolated dark solitons . We find that the gain is generally higher for a dark soliton located near the switching front ( Fig3a ) than for a dark soliton in ...
Contents
L Lasers and Resonators | 1 |
Compact electricdischarge excimer lasers invited | 14 |
Simplified model for XECLlasers | 29 |
Copyright | |
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