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1.
Opt Lett ; 34(14): 2165-7, 2009 Jul 15.
Artigo em Inglês | MEDLINE | ID: mdl-19823536

RESUMO

We study the generation of intense terahertz pulses produced by two-color laser pulse filamentation in air. We tailor the filamentation process and the produced plasma strings and study how the generated terahertz field is modified. An important terahertz pulse shortening is found for plasma strings with uniform electron density.

2.
Opt Lett ; 33(24): 3028-30, 2008 Dec 15.
Artigo em Inglês | MEDLINE | ID: mdl-19079530

RESUMO

We exploit cross-phase modulation by a strong driving pulse onto a weaker probe pulse at a different wavelength to induce the formation of an X wave possessing the typical nondispersive and nondiffractive propagation properties.

3.
Opt Express ; 16(11): 8213-8, 2008 May 26.
Artigo em Inglês | MEDLINE | ID: mdl-18545532

RESUMO

We study the effect of Two-Photon Absorption (TPA) nonlinear losses on Gaussian pulses, with power that exceeds the critical power for self-focusing, propagating in bulk kerr media. Experiments performed in fused silica and silicon highlight a spontaneous reshaping of the input pulse into a pulsed Bessel beam. A filament is formed in which sub-diffractive propagation is sustained by the Bessel-nature of the pulse.


Assuntos
Refratometria/métodos , Simulação por Computador , Luz , Modelos Teóricos , Fótons , Espalhamento de Radiação
4.
Opt Express ; 15(20): 13077-95, 2007 Oct 01.
Artigo em Inglês | MEDLINE | ID: mdl-19550576

RESUMO

Focus Serial: Frontiers of Nonlinear Optics

We investigate ultrashort laser pulse filamentation within the framework of spontaneous X Wave formation. After a brief overview of the filamentation process we study the case of an intense filament co-propagating with a weaker seed pulse. The filament is shown to induce strong Cross-Phase-Modulation (XPM) effects on the weak seed pulse: driven by the pump, the seed pulse undergoes pulse splitting with the daughter pulses slaved to their pump counterparts. They undergo strong spatio-temporal reshaping and are transformed into XWaves traveling at the same group velocities as the pump split-off pulses. In the presence of a gain mechanism such as Four-Wave-Mixing or Stimulated Raman Scattering, energy is then transferred from the pump filament leading to amplification of the seed X Wave and formation of a temporally compressed intensity peak.

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