2016
DOI: 10.1109/jlt.2016.2624699
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Role of the Input Profile Asymmetry and the Chirp on the Propagation in Highly Dispersive and Nonlinear Fibers

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Cited by 17 publications
(16 citation statements)
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“…The truncation coefficient or decay factor 𝑎 (0 < 𝑎 < 1) is a quantity to ensure containment of the infinite Airy tail and can thus enable the physical realization of such pulses [36]. In practice, an Airy pulse can be produced by adding a cubic phase to a Gaussian spectrum [7,35,36]. The truncation coefficient is taken as 𝑎 = 0.05.…”
Section: Modellingmentioning
confidence: 99%
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“…The truncation coefficient or decay factor 𝑎 (0 < 𝑎 < 1) is a quantity to ensure containment of the infinite Airy tail and can thus enable the physical realization of such pulses [36]. In practice, an Airy pulse can be produced by adding a cubic phase to a Gaussian spectrum [7,35,36]. The truncation coefficient is taken as 𝑎 = 0.05.…”
Section: Modellingmentioning
confidence: 99%
“…In the SCG studies, the overwhelming majority of prior studies already cited above [1][2][3][4][5][6]8,9] utilized intense optical pulses with symmetric and compact temporal profiles such as Gaussian or sech-type pulses while the only ones that focused on Airy pulses are those of refs. [7,10,11,13]. One should remind that, Airy pulses are first predicted by Berry and Balazs within the context of quantum mechanics [14] and, their first introduction in nonlinear optics followed in 2007 by Siviloglou and Christodoulides [15].…”
Section: Introductionmentioning
confidence: 98%
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