2011
DOI: 10.1103/physreva.84.063838
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Understanding the dynamics of photoionization-induced nonlinear effects and solitons in gas-filled hollow-core photonic crystal fibers

Abstract: We present the details of our previously formulated model [Saleh et al., Phys. Rev. Lett. 107, 203902 (2011)] that governs pulse propagation in hollow-core photonic crystal fibers filled by an ionizable gas. By using perturbative methods, we find that the photoionization process induces the opposite phenomenon of the well-known Raman self-frequency redshift of solitons in solid-core glass fibers, as was recently experimentally demonstrated [Holzer et al., Phys. Rev. Lett. 107, 203901 (2011)]. This process is o… Show more

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Cited by 32 publications
(32 citation statements)
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“…Therefore, in HCPCF this phenomenon appears for lower laser average power values than the one required in simple capillaries in high field domain. This ionization process is intrinsically linked to a loss decrease [129,130].…”
Section: Photo-induced Plasmamentioning
confidence: 99%
See 1 more Smart Citation
“…Therefore, in HCPCF this phenomenon appears for lower laser average power values than the one required in simple capillaries in high field domain. This ionization process is intrinsically linked to a loss decrease [129,130].…”
Section: Photo-induced Plasmamentioning
confidence: 99%
“…Good agreement has been obtained between experiments and numerical simulations when an ionization term is taken into account in the model in term of spectral evolution and also in the energy losses. Further, the theoretical explanations of this blue-shift effect have been deeply developed in References [130,134].…”
Section: Photo-induced Plasmamentioning
confidence: 99%
“…The model introduced in [4,5] for pulse propagation in nonlinear gaseous media presenting Kerr and plasma nonlinearities has the following dimensionless version i ∂q ∂ξ + 1 2…”
Section: One Parameter Ode and Perturbation Approachmentioning
confidence: 99%
“…, where k 0 = ω 0 /c with c being the speed of light and ω 0 is the input pulse central frequency, σ is related to two constants [14], ω T is the maximum plasma frequency, A eff is the effective mode area and γ K is the nonlinear Kerr coefficient of the gas.…”
Section: Introductionmentioning
confidence: 99%