Modulation instability of bright photovoltaic solitons on a partially incoherent background

Zhang, M.; Huo, Guangwen; Zhang, Y.; Kang, Yifan; Duan, Zhenglu

doi:10.1134/s1054660x12080178

Cited by 5 publications

(1 citation statement)

References 24 publications

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“…Properties of the optical spatial solitons in the photorefractive crystals with emphasis to two-photon photorefractive nonlinearity have been studied [6]. Modulation instability of the bright photovoltaic solitons on a partially incoherent background and incoherently coupled bright-dark photovoltaic soliton pairs based on two-photon photorefractive effect have been investigated [7,8]. Dynamic and steadystate behavior of optical solitons propagating in nematic liquid crystals have been discussed [9].…”

Section: Introductionmentioning

confidence: 99%

Dynamic behavior of the incoherent optical spatial solitons in a nonlocal nonlinear medium

Zhen

Tian

Xie

et al. 2015

Journal of Modern Optics

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Dynamic behavior of the propagation of incoherent optical spatial solitons in a nonlocal nonlinear medium is investigated. By means of the Hirota method, we obtain the soliton solutions, based on which we find that |ψ| is positively related to n 0 , but inversely related to ω and κ, whereas n is independent of them, with ψ as the slowly varying amplitude of the beam, n as the refractive index change, n 0 , ω, and κ as the unperturbed refractive index, frequency of the propagating beam, and beam intensity distribution, respectively. Head-on and bound-state soliton interactions are both given, and one interaction period decreases with ω and κ increasing in the bound state one. With the external perturbations taken into consideration, the associated chaotic motions of the perturbed model are studied, and the corresponding power spectra and phase projections are obtained. Both the weak and developed chaotic states are investigated, and the difference between them roots in the relative magnitude of nonlinearities and perturbations. Such chaotic motions can be weakened via increasing ω and κ or decreasing n 0 . Periodic motion is obtained with the nonlinearities and perturbations balanced.

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