2008
DOI: 10.1007/s00340-008-2959-9
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Optimization of a femtosecond pulse self-compression region along a filament in air

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Cited by 54 publications
(23 citation statements)
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“…2). This results are in a good agreement with experiments [24] and simulation [29] of self-compression in femtosecond filament. According to the stationary theory (1, 7) signal pulse wavelength λ2 is equal to 8.4 μm (λ1 = 420 nm), 3.6 μm (λ1 = 450 nm) и 2.4 μm (λ1 = 480 nm).…”
Section: Introductionsupporting
confidence: 93%
“…2). This results are in a good agreement with experiments [24] and simulation [29] of self-compression in femtosecond filament. According to the stationary theory (1, 7) signal pulse wavelength λ2 is equal to 8.4 μm (λ1 = 420 nm), 3.6 μm (λ1 = 450 nm) и 2.4 μm (λ1 = 480 nm).…”
Section: Introductionsupporting
confidence: 93%
“…This conclusion is conérmed in paper [187], where the pulse duration after élamentation in a VK7 glass decreased from 50 to 20 fs. The authors of [188] determined the region of a élament for collimated radiation in air where the maximum compression of a pulsed was achieved. It was shown that the duration of a 805-nm, 55-fs, 4-mJ pulse under these conditions decreased to 9 fs.…”
Section: Pulse Compressionmentioning
confidence: 99%
“…Considerable success has recently been achieved in self-compression of femtosecond laser pulses in gases. It has been shown both experimentally and theoretically [2][3][4][5][6] that the initial several-tensof-femtoseconds-long pulses can be compressed down to almost one oscillation cycle. Using such extremely compressed IR pulses, attosecond pulses in the UV can be obtained in the process of high-order harmonic generation [7,8].…”
Section: Introductionmentioning
confidence: 99%