2019
DOI: 10.1088/1402-4896/ab2e89
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Effects of delayed Kerr nonlinearity on the propagation of femtosecond annular Gaussian filaments in air

Abstract: The effects of the delayed Kerr nonlinearity on the annular Gaussian filaments nearby the characteristic time of the molecular rotational respond are numerically investigated. The simulated results show that the delayed Kerr nonlinearity leads to the advancement of the filament onset distance when the pulse duration is fixed. Moreover, in the presence of the delayed Kerr nonlinearity, the length of the filament is obviously extended, and the peak plasma density appears the great oscillations that makes the fil… Show more

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Cited by 5 publications
(1 citation statement)
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“…In order to adequately understand the influences of input pulse energy on the characteristics of laser filaments, figure 7 shows the simulated dependence of various filamentation parameters including length of filament (L f ), maximum electron density (ρ max ), peak fluence (F max ), total deposited energy (ΔE), maximum energy deposition rate ( / ¶D ¶ E z), and maximum local temperature variation (ΔT) as a function of input energy. Here, we define the filament length as the length from the onset distance to the value of the peak plasma density less than 10 14 cm −3 at the last beam collapse [37]. As shown in figure 7(a), the increase of filament length is limited by the formation of multiple filaments with the growth of the pulse energy.…”
Section: Characteristics Of Heat Depositionmentioning
confidence: 99%
“…In order to adequately understand the influences of input pulse energy on the characteristics of laser filaments, figure 7 shows the simulated dependence of various filamentation parameters including length of filament (L f ), maximum electron density (ρ max ), peak fluence (F max ), total deposited energy (ΔE), maximum energy deposition rate ( / ¶D ¶ E z), and maximum local temperature variation (ΔT) as a function of input energy. Here, we define the filament length as the length from the onset distance to the value of the peak plasma density less than 10 14 cm −3 at the last beam collapse [37]. As shown in figure 7(a), the increase of filament length is limited by the formation of multiple filaments with the growth of the pulse energy.…”
Section: Characteristics Of Heat Depositionmentioning
confidence: 99%