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 4
... operation is achieved by inserting phase elements within the laser resonator , so as to introduce high losses to the undesired modes and low losses to the desired mode [ 7 ] . Once a single high order mode beam is obtained , with well ...
... operation is achieved by inserting phase elements within the laser resonator , so as to introduce high losses to the undesired modes and low losses to the desired mode [ 7 ] . Once a single high order mode beam is obtained , with well ...
Page 12
... operation of the optically coupled lasers in Refs.6,7 were studied . I , arb . un . 2 1 100 200 300 F , kHz Figure 4 Spectrum of a chaotic signal in a system of two optically coupled lasers . 1 ' W1 , arb . un . 1- 2 ' W2 , arb . un ...
... operation of the optically coupled lasers in Refs.6,7 were studied . I , arb . un . 2 1 100 200 300 F , kHz Figure 4 Spectrum of a chaotic signal in a system of two optically coupled lasers . 1 ' W1 , arb . un . 1- 2 ' W2 , arb . un ...
Page 107
... operation temperature growth , the threshold of the long - wavelength lasers increases mainly because of Auger recombination ( AR ) enhancement [ 1 ] . High performance is available for laser diodes on asymmetric quantum - well ( QW ) ...
... operation temperature growth , the threshold of the long - wavelength lasers increases mainly because of Auger recombination ( AR ) enhancement [ 1 ] . High performance is available for laser diodes on asymmetric quantum - well ( QW ) ...
Contents
L Lasers and Resonators | 1 |
Compact electricdischarge excimer lasers invited | 14 |
Simplified model for XECLlasers | 29 |
Copyright | |
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