Proceedings of Topical Meeting on Optoinformatics (pdf-format, 1.21 ...
Proceedings of Topical Meeting on Optoinformatics (pdf-format, 1.21 ...
Proceedings of Topical Meeting on Optoinformatics (pdf-format, 1.21 ...
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SAINT-PETERSBURG, October 17 – 20, 2005 65<br />
GENERATION OF THE DISCRETE SPECTRAL<br />
SUPERCONTINUUM IN TWO INTENSIVE ULTRASHORT PULSES<br />
INTERACTION<br />
M. A. Bakhtin, S. A. Kozlov<br />
St.Petersburg State University <str<strong>on</strong>g>of</str<strong>on</strong>g> In<strong>format</strong>i<strong>on</strong> Technologies, Mechanics and Optics<br />
Kr<strong>on</strong>verksky pr. 49, St.Petersburg, 197101, Russia<br />
E-mail: bakhtin@rain.ifmo.ru<br />
It is shown that n<strong>on</strong>linear interacti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> two intensive few-cycle pulses in<br />
waveguide can result in high repetiti<strong>on</strong> rate optical sequence generati<strong>on</strong> with<br />
quasi-discrete spectrum that can be used for in<strong>format</strong>i<strong>on</strong> encoding.<br />
The fiber optical systems have gained more and more popularity for data<br />
transmissi<strong>on</strong>. Wave density multiplexing systems are widely used now to achieve high<br />
bandwidths for optical channels. Current WDM implementati<strong>on</strong>s require many optical<br />
sources (<strong>on</strong>e for every channel). In present paper we c<strong>on</strong>sider a method <str<strong>on</strong>g>of</str<strong>on</strong>g> generati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
very high frequency optical signal sequence based <strong>on</strong> interacti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> two few-cycle laser<br />
pulses propagating collinearly in transparent n<strong>on</strong>linear media with different group<br />
velocities. The spectrum <str<strong>on</strong>g>of</str<strong>on</strong>g> generated sequence is quasi-discrete that allows using it as<br />
multiple light sources with different wavelengths. Fig. 1 dem<strong>on</strong>strates the interacti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the<br />
two few-cycle pulses with central wavelengths 780 nm and 390 nm with input intensities<br />
2·10 13 W/cm 2 in fused silica.<br />
Fig. 1. Spatial evoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> electric field envelope ε ( z , t ) for the pulses interacti<strong>on</strong> with peak<br />
input intensity I 1 =I 2 =2·10 13 W/cm 2<br />
Fig. 2. Quasi-discrete spectrum <str<strong>on</strong>g>of</str<strong>on</strong>g> generated sequence<br />
The interacti<strong>on</strong> was modeled by n<strong>on</strong>linear equati<strong>on</strong>s describing the temporal<br />
evoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> light pulse electrical fields and their spatial - temporal spectra up<strong>on</strong> the pulses