2015
DOI: 10.1103/physreve.92.042915
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Rodlike localized structure in isotropic pattern-forming systems

Abstract: Stationary two-dimensional localized structures have been observed in a wide variety of dissipative systems. The existence, stability properties, dynamical evolution, and bifurcation diagram of an azimuthal symmetry breaking, rodlike localized structure in the isotropic prototype model of pattern formation, the Swift-Hohenberg model, is studied. These rodlike structures persist under the presence of nongradient perturbations. Interaction properties of the rodlike structures are studied. This allows us to envis… Show more

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Cited by 11 publications
(6 citation statements)
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References 52 publications
(61 reference statements)
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“…We have found no evidence for the coexistence of this state with any spatially extended state at these parameter values. Note that dumbbell localized states were previously observed in the classical nonconserved SH equation in both 2D and 3D [112]. Next, we move on to the active PFC model and investigate the influence of the activity parameter v 0 .…”
Section: Localized Statesmentioning
confidence: 92%
“…We have found no evidence for the coexistence of this state with any spatially extended state at these parameter values. Note that dumbbell localized states were previously observed in the classical nonconserved SH equation in both 2D and 3D [112]. Next, we move on to the active PFC model and investigate the influence of the activity parameter v 0 .…”
Section: Localized Statesmentioning
confidence: 92%
“…Figure 3 depicts the bifurcation diagram of Eq. (2) as function of the parameter η (for details of the bifurcation diagram see refs 22,24,27 ). The vertical axis accounts for the amplitude || A || of the pattern.…”
Section: Resultsmentioning
confidence: 99%
“…Several physical effect have been proposed in the literature such as Kerr cavities [17][18][19] . The existence of stable LBs have been reported in other systems such as in wide-aperture lasers with a saturable absorber [20][21][22][23][24] , optical parametric oscillators [25][26][27] , second harmonic generation [28,29] , passively mode-locked semiconductor lasers [30] , left-handed materials [31] , twisted waveguide arrays [32] , in Swif-Hohenberg equation [25,28,33] , and in the complex cubic-quintic Ginzburg-Landau equation [34] . (see recent reviews [35][36][37] ).…”
Section: Introductionmentioning
confidence: 95%