2003
DOI: 10.1364/ol.28.001591
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Optical breakdown versus filamentation in fused silica by use of femtosecond infrared laser pulses

Abstract: The competition between optical breakdown (OB) and laser-pulse filamentation (FL) in bulk fused silica is investigated by using a 1-kHz femtosecond infrared laser. We measure input powers corresponding to the threshold of OB and FL in terms of external focusing conditions. The results demonstrate that OB precedes FL for tight focusing, whereas for sufficiently long focal lengths FL takes places at a lower power than OB does.

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Cited by 110 publications
(45 citation statements)
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“…A typical SC spectrum produced in fused silica extends from 390 to 1000 nm, as reported under various experimental conditions [131,132,[146][147][148][149]. Although similar, but somewhat narrower SC spectra were generated in BK7 [146,150,151] and ZK7 [152] glasses, which possess smaller bandgaps.…”
Section: Glassessupporting
confidence: 65%
See 1 more Smart Citation
“…A typical SC spectrum produced in fused silica extends from 390 to 1000 nm, as reported under various experimental conditions [131,132,[146][147][148][149]. Although similar, but somewhat narrower SC spectra were generated in BK7 [146,150,151] and ZK7 [152] glasses, which possess smaller bandgaps.…”
Section: Glassessupporting
confidence: 65%
“…These practical issues are universal and hold for any nonlinear medium and at any input wavelength in the optical range. First of all, the optical damage of the medium is the major limiting factor in SC generation, therefore the external focusing condition (the numerical aperture, NA) should be carefully chosen [131,132]. Figure 7 shows the experimentally measured threshold energies for SC generation and optical damage in fused silica as functions of the numerical aperture [132].…”
Section: Practical Considerationsmentioning
confidence: 99%
“…However, for self-trapping of the laser beam over a length of several millimetres, the incident peak power needs to be significantly larger than the threshold for critical self-focusing. The length and threshold for a filament depends on the focusing conditions [106]. Loose focusing shows larger thresholds but results in longer filaments [107].…”
Section: Kerr Self-focusingmentioning
confidence: 99%
“…Exceeding the critical power results in self-focusing and laser-pulse filamentation. 3 Recently, femtosecond laser pulses have been used to write three-dimensional waveguide structures in a variety of bulk glass samples. 4,5 Furthermore, long period gratings 6 as well as fiber Bragg gratings 7 have been realized by modification of the core index in germanosilicate fibers.…”
mentioning
confidence: 99%