1998
DOI: 10.1016/s0375-9601(98)00532-5
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Analysis of stable self-trapping of laser beams in cubic-quintic nonlinear media

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Cited by 60 publications
(34 citation statements)
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“…That is why its simplest version, the CQ nonlinearity, attracts significant attention of theoreticians from the early days of nonlinear optics (Zakharov, Sobolev, and Synakh [1971]). Numerical studies have confirmed the stability of fundamental spatial solitons in this system (Wright, Lawrence, Torruellas, and Stegeman [1995]; Dimitrevski, Reimhult, Svensson, Ohgren, Anderson, Berntson, Lisak, and Quiroga-Teixeiro [1998]; Quiroga-Teixeiro, Berntson, and Michinel [1999]). Experimentally a CQ nonlinear dielectric response with positive cubic and negative quintic contributions has been observed in chalcogenide glasses (Smektala, Quemard, Couderc, and Barthelemy [2000]; Boudebs, Cherukulappurath, Leblond, Troles, Smektala, and Sanchez [2003]), and in organic materials (Zhan, Zhang, Zhu, Wang, Li, Li, Lu, Zhao, and Nie [2002]).…”
Section: Cubic-quintic Nonlinearitysupporting
confidence: 52%
“…That is why its simplest version, the CQ nonlinearity, attracts significant attention of theoreticians from the early days of nonlinear optics (Zakharov, Sobolev, and Synakh [1971]). Numerical studies have confirmed the stability of fundamental spatial solitons in this system (Wright, Lawrence, Torruellas, and Stegeman [1995]; Dimitrevski, Reimhult, Svensson, Ohgren, Anderson, Berntson, Lisak, and Quiroga-Teixeiro [1998]; Quiroga-Teixeiro, Berntson, and Michinel [1999]). Experimentally a CQ nonlinear dielectric response with positive cubic and negative quintic contributions has been observed in chalcogenide glasses (Smektala, Quemard, Couderc, and Barthelemy [2000]; Boudebs, Cherukulappurath, Leblond, Troles, Smektala, and Sanchez [2003]), and in organic materials (Zhan, Zhang, Zhu, Wang, Li, Li, Lu, Zhao, and Nie [2002]).…”
Section: Cubic-quintic Nonlinearitysupporting
confidence: 52%
“…For larger values of the propagation constant, the beam flux grows rapidly with β and the peak amplitude of the distribution saturates due to the effect of n 4 , reaching asymptotically the value A cr which is slightly below the maximum amplitude. Thus, high power beams show spatial light distributions with flatted tops in their profiles, similar to those of hyper-Gaussian functions [24,25]. We must stress the intriguing fact that both β cr and A cr do not depend on the value of the topological charge.…”
Section: Introductionmentioning
confidence: 74%
“…To explain the properties of the above light distributions, we have performed a variational analysis [24,25].…”
Section: Variational Analysismentioning
confidence: 99%
“…On the other hand, the theoretical description of these localized modes is in general based on nonlinear Schrödinger equations (NLSE) [6][7][8]. In the modeling of these kind of systems, nonlinear effects like two and three photon absorption, second order group-velocity dispersion, time-delayed nonlinear response, multiphoton ionization and plasma defocusing [9] are usually taken into account.…”
Section: Introductionmentioning
confidence: 99%