Evolution of airy pulses in the present of third order dispersion

Cai, Wangyang; Wang, Lei; Wen, Shuangchun

doi:10.1016/j.ijleo.2013.04.043

Cited by 17 publications

(13 citation statements)

References 9 publications

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“…For an Airy pulse with a multipeak structure, the width of its main lobe is typically used as a temporal scale. [37,46] Then, the profile of an Airy pulse at any point Z along the propagation direction can be given by [35] A (Z,…”

Section: Theoretical Modelmentioning

confidence: 99%

“…The propagation of truncated Airy pulses can be controlled by dispersion, nonlinearity, initial frequency chirping, and time-varying optical potentials. [35][36][37][38][39][40][41] The interactions between Airy pulses and solitons present novel dynamics. Temporal soliton interactions with a truncated Airy pulse can be controlled via the initial phase, amplitude, and time position of the Airy pulse.…”

Section: Introductionmentioning

confidence: 99%

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Reflection and Refraction of an Airy Pulse at a Moving Temporal Boundary

et al. 2020

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Reflection and refraction of Airy pulses at a moving step refractive-index boundary are investigated. A comb-like reflected spectrum and an Airy-like transmitted spectrum are formed as an Airy pulse crosses a temporal boundary without initial group velocity mismatch or initial central frequency shift. The reflected and refracted pulses are significantly influenced by the location of temporal boundary and time-dependent refractive index change. The energy of each lobe of the comb-like reflected spectra can be controlled by changing the value of decay factor of the Airy pulse. In the case of an Airy pulse with an initial launch frequency shift, the reflected and refracted frequency shifts depend on the dispersion relation of the medium. The results can be used in potential applications involving optical manipulation.

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Section: Theoretical Modelmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Reflection and Refraction of an Airy Pulse at a Moving Temporal Boundary

et al. 2020

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“…(4). Once this is done, the resulting pulse propagating in the second-and third-order dispersion medium is given by Eq.…”

Section: Theoretical Description Of Airy-type Pulses Truncated In Timementioning

confidence: 99%

“…However, it is possible to obtain a finite-energy version of the ideal Airy pulse by modulating it with a time exponential function on the initial plane z 0 [2,3]. The analysis of a finite-energy Airy pulse considering the effects of second-and third-order dispersion was first made in [3] and subsequently in [4][5][6]. Additional work on finiteenergy Airy beams and pulses is provided in Refs.…”

Section: Introductionmentioning

confidence: 99%

Propagation of time-truncated Airy-type pulses in media with quadratic and cubic dispersion

et al. 2015

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In this paper, we describe analytically the propagation of Airy-type pulses truncated by a finite-time aperture when second- and third-order dispersion effects are considered. The mathematical method presented here, which is based on the superposition of exponentially truncated Airy pulses, is very effective and allows us to avoid the use of time-consuming numerical simulations. We analyze the behavior of the time-truncated ideal Airy pulse and also the interesting case of a time-truncated Airy pulse with a "defect" in its initial profile, which reveals the self-healing property of this kind of pulse solution.

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“…It can also be produced by imparting a cubic spectral phase on an incident pulse through other pulse shaping techniques 21 . Extensive studies have been devoted to disclose the propagation dynamics of truncated Airy pulse from linear 10 11 18 22 23 24 25 26 to nonlinear 27 28 29 30 31 32 33 34 35 regimes. In linear optics, it was used for the realization of linear spatiotemporal light bullets 10 11 .…”

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confidence: 99%

Engineering deceleration and acceleration of soliton emitted from Airy pulse with quadratic phase modulation in optical fibers without high-order effects

Zhang

Liu

Zhong

et al. 2015

Sci Rep

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Soliton propagation direction can be engineered in optical fibers in the presence of high-order effects (HOEs). It is well known that Raman effects can decelerate the soliton. Here we investigate the manipulation of the deceleration or acceleration of soliton emitted from Airy pulse whose spectrum is imposed an initial quadratic phase modulation (QPM) in optical fibers in the absence of HOEs. We show that, under the action of the anomalous second-order dispersion (SOD) and Kerr nonlinearity, Airy pulse with QPM is able to emit soliton with acceleration or deceleration depending on whether the QPM is negative or positive, and at a rate that is determined by the magnitude of QPM. The reason is that the acceleration behaviors of incident Airy pulse is altered depending on whether SOD and QPM have the same or opposite signs. Our study shows the possibility of controlling and manipulating the soliton propagation and interaction in optical fibers without HOEs, by purposely choosing appropriate QPM parameter of an Airy pulse.

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Evolution of airy pulses in the present of third order dispersion

Cited by 17 publications

References 9 publications

Reflection and Refraction of an Airy Pulse at a Moving Temporal Boundary

Reflection and Refraction of an Airy Pulse at a Moving Temporal Boundary

Propagation of time-truncated Airy-type pulses in media with quadratic and cubic dispersion

Engineering deceleration and acceleration of soliton emitted from Airy pulse with quadratic phase modulation in optical fibers without high-order effects

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