2016
DOI: 10.1038/srep20363
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Dramatic enhancement of supercontinuum generation in elliptically-polarized laser filaments

Abstract: Broadband laser sources based on supercontinuum generation in femtosecond laser filamentation have enabled applications from stand-off sensing and spectroscopy to the generation and self-compression of high-energy few-cycle pulses. Filamentation relies on the dynamic balance between self-focusing and plasma defocusing – mediated by the Kerr nonlinearity and multiphoton or tunnel ionization, respectively. The filament properties, including the supercontinuum generation, are therefore highly sensitive to the pro… Show more

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Cited by 35 publications
(10 citation statements)
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References 34 publications
(72 reference statements)
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“…However, the change in the beams polarization itself as a result of its collapse remains largely unexplored. Since several applications of laser filamentation including HHG, THz generation and supercontinuum generation are polarization sensitive [38][39][40], investigating the polarization state of collapsing beams is crucial [41][42][43]. In some of the studies, molecular alignment and delayed birefringence acting on the probe were investigated [44][45][46].…”
Section: Introductionmentioning
confidence: 99%
“…However, the change in the beams polarization itself as a result of its collapse remains largely unexplored. Since several applications of laser filamentation including HHG, THz generation and supercontinuum generation are polarization sensitive [38][39][40], investigating the polarization state of collapsing beams is crucial [41][42][43]. In some of the studies, molecular alignment and delayed birefringence acting on the probe were investigated [44][45][46].…”
Section: Introductionmentioning
confidence: 99%
“…The intensity of the emission is determined by the gain and the continuum available to seed it, so it is important to consider the continuum in this context. Continuum generation strongly depends on laser ellipticity [32] and will influence the emission if the gain is not saturated. The continuum is highlighted in Figure 3(a), where the spectrum is separated into three regions: the ion emission at 428 nm, continuum next to the ion emission (431 -455 nm), and continuum far from the ion emission (479 -531 nm).…”
mentioning
confidence: 99%
“…For instance, a strong backward stimulated radiation at 337 nm has been observed from a filament in nitrogen gas driven by a circularly polarized femtosecond laser pulse centered at 800 nm [19] . Filament-induced supercontinuum generation in molecular gases was dramatically enhanced in elliptically-polarized laser filaments [20] . Numerical simulations of the formation and development of filaments in argon with close to linear or circular polarization pulses [17] , polarization-dependent supercontinuum generation during filamentation [21] , and multiple filamentation suppression with circularly polarized pulses [22] have been reported.…”
mentioning
confidence: 99%