2014
DOI: 10.1103/physreva.89.033809
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Whole life cycle of femtosecond ultraviolet filaments in water

Abstract: International audienceWe present measurements fully characterizing the whole life cycle of femtosecond pulses undergoing filamentation in water at 400 nm. The complete pulse dynamics is monitored by means of a four-dimensional mapping technique for the intensity distribution I(x,y,z,t) during the nonlinear interaction. Measured events (focusing or defocusing cycles, pulse splitting and replenishment, supercontinuum generation, conical emission, nonlinear absorption peaks) are mutually connected.The filament ev… Show more

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Cited by 44 publications
(19 citation statements)
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“…With the ultraviolet pump pulses generated by the frequency doubling of an amplified Ti:sapphire laser output, the measured SC spectra covered wavelength ranges of 290-530 nm [146] and 350-550 nm [138], as reported with pump wavelengths of 393 and 400 nm, respectively, and under slightly different external focusing conditions. With the pump wavelengths in the visible spectral range, the SC spectrum from 400 to 650 nm was generated with 527 nm self-compressed femtosecond second harmonic pulses from the Nd:glass laser [175] and from 450 to 720 nm with 594 nm pulses from a rhodamine 6G dye laser [11].…”
Section: Watermentioning
confidence: 99%
See 1 more Smart Citation
“…With the ultraviolet pump pulses generated by the frequency doubling of an amplified Ti:sapphire laser output, the measured SC spectra covered wavelength ranges of 290-530 nm [146] and 350-550 nm [138], as reported with pump wavelengths of 393 and 400 nm, respectively, and under slightly different external focusing conditions. With the pump wavelengths in the visible spectral range, the SC spectrum from 400 to 650 nm was generated with 527 nm self-compressed femtosecond second harmonic pulses from the Nd:glass laser [175] and from 450 to 720 nm with 594 nm pulses from a rhodamine 6G dye laser [11].…”
Section: Watermentioning
confidence: 99%
“…The general interpretation of focusing/refocusing cycles is based on the socalled dynamic spatial replenishment scenario, which assumes alternating cycles of self-focusing due to the Kerr effect and self-defocusing due to free electron plasma and which was originally proposed to explain the illusion of long-distance selfguided propagation of high-power pulses in gaseous media [137]. A more recent experimental and numerical study of the full spatiotemporal evolution of light filaments versus the propagation distance in water unveiled the intimate connections between complex propagation effects: focusing and refocusing cycles, nonlinear absorption, pulse splitting and replenishment, supercontinuum generation and conical emission [138]. More specifically, whenever the self-focusing wave packet (the ultrashort pulsed laser beam) approaches the nonlinear focus, multiphoton absorption attenuates its central part, which after the pulse splitting is reshaped into a ring-like structure.…”
Section: Practical Considerationsmentioning
confidence: 99%
“…[35][36][37] Indeed, hot spots in the central part of the beam corresponding to filament formation were directly observed in our experiments, while the radial lobes had intensities too low to produce a filament as seen in the image of the inset of Fig. 1.…”
Section: Experimental Details Results and Discussionmentioning
confidence: 75%
“…However, due to the severe distortion of the laser pulse during nonlinear propagation and ionization, complete characterization of spatiotemporal intensity distribution is extremely difficult and such measurements have so far been restricted to filamentation in short water cells. 39 Indirect estimations 40 have shown that the maximum laser intensity in femtosecond filaments in 1 atm air is clamped at the order of $10 13 W/cm 2 .…”
Section: B Measurement Of Electron Density In a Femtosecond Filamentmentioning
confidence: 99%