2011
DOI: 10.1063/1.3657774
|View full text |Cite
|
Sign up to set email alerts
|

Kerr-driven nonlinear refractive index of air at 800 and 400 nm measured through femtosecond laser pulse filamentation

Abstract: The filamentation dynamics of 15 GW femtosecond laser pulses at 800 and 400 nm wavelengths upon their tight focusing in air is studied experimentally. The spatial position and extent of plasma channel formed within the filamentation zone as a function of laser pulse power are investigated. The processing of the experimental data according to the Marburger formula by J. H. Marburger [Prog. Quantum. Electron. 4, 35 (1975)] and the dispersion relations for air cubic nonlinearity has allowed to estimate the effect… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
14
0

Year Published

2013
2013
2021
2021

Publication Types

Select...
10

Relationship

1
9

Authors

Journals

citations
Cited by 37 publications
(15 citation statements)
references
References 14 publications
1
14
0
Order By: Relevance
“…(2-6) with the relevant pulse duration and energies, and with a fit of B xxxx = 2.36 × 10 −7 cm 3 /erg • s, B ′ xxxx = 2.58 × 10 −7 cm 3 /erg • s and τ n = 14.2 ps. The third-order nonlinear susceptibility χ (3) can be estimated by χ (3) ≈ 3B xxxx τ n = 1.006 × 10 −17 cm 3 /erg, and then the delayed nonlinear refractive index coefficient n 2,d = 12π 2 χ (3) /n 2 0 c = 3.97 × 10 −19 cm 2 /W , which is close to the reported value of ∼ 3.01 × 10 −19 cm 2 /W in literature 20,21 . The fit in Fig.…”
Section: Fig 2 (Color Online)supporting
confidence: 87%
“…(2-6) with the relevant pulse duration and energies, and with a fit of B xxxx = 2.36 × 10 −7 cm 3 /erg • s, B ′ xxxx = 2.58 × 10 −7 cm 3 /erg • s and τ n = 14.2 ps. The third-order nonlinear susceptibility χ (3) can be estimated by χ (3) ≈ 3B xxxx τ n = 1.006 × 10 −17 cm 3 /erg, and then the delayed nonlinear refractive index coefficient n 2,d = 12π 2 χ (3) /n 2 0 c = 3.97 × 10 −19 cm 2 /W , which is close to the reported value of ∼ 3.01 × 10 −19 cm 2 /W in literature 20,21 . The fit in Fig.…”
Section: Fig 2 (Color Online)supporting
confidence: 87%
“…The multiphoton photoionization rate I W is calculated using the Perelomov-Popov-Terent'ev model [46], which is applied to a gas mixture simulating atmospheric air (20%O 2 +80%N 2 ) at the total neutral molecule concentration of 2.5•10 19 cm -3 . The critical self-focusing power c P of laser radiation at the wavelength of 800 nm in air is set as 3.2 GW [47].…”
Section: Fundingmentioning
confidence: 99%
“…depending on the propagation direction. The calculation shows that the nonlinear refractive index of vacuum (n 2,vac = 1.36 × 10 −29 cm 2 /W for n 2,vac = 4κ/c 0 ) is 3 × 10 10 times lower than that of air (n 2,air = 4 × 10 −19 cm 2 /W) at 800 nm wavelength [52] and 10 19 times lower than that of water [53].…”
Section: A Nonlinear Birefringent Vacuum Induced By the Transverse Magnetic Mode Fieldmentioning
confidence: 92%