2015
DOI: 10.1134/s1024856015030033
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Multiple filamentation of collimated Ti:Sapphire laser beams in water

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Cited by 2 publications
(2 citation statements)
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“…Note that for the same parameters, simple use of the Marburger formula [19] incorrectly predicts L SF = 2 m for the collapse-, or filament onset-length in water. Our result is in agreement with the experiments performed by Apeximov et al [20], who find that their collimated beam with similar properties produces single filaments at P in ∼ 3100 P NL in water, and multiple filaments at higher powers. Table I shows the filament probability p(≥ 1), the probability of the laser shot producing one or more filaments, for different values of C 2 n at distance z = 18 cm.…”
Section: Resultssupporting
confidence: 93%
See 1 more Smart Citation
“…Note that for the same parameters, simple use of the Marburger formula [19] incorrectly predicts L SF = 2 m for the collapse-, or filament onset-length in water. Our result is in agreement with the experiments performed by Apeximov et al [20], who find that their collimated beam with similar properties produces single filaments at P in ∼ 3100 P NL in water, and multiple filaments at higher powers. Table I shows the filament probability p(≥ 1), the probability of the laser shot producing one or more filaments, for different values of C 2 n at distance z = 18 cm.…”
Section: Resultssupporting
confidence: 93%
“…At a pulse power of P in = 14.2 GW and in an unperturbed atmosphere, filaments are absent in the watercell. This may seem surprising as the incident power widely exceeds the P NL,water = 6.5 MW [20] for λ = 800 nm. Indeed, experiments in water are commonly performed at much lower power.…”
Section: Resultsmentioning
confidence: 99%