Search results for " 34C05"

showing 3 items of 3 documents

Multiplicity of fixed points and growth of ε-neighborhoods of orbits

2012

We study the relationship between the multiplicity of a fixed point of a function g, and the dependence on epsilon of the length of epsilon-neighborhood of any orbit of g, tending to the fixed point. The relationship between these two notions was discovered before (Elezovic, Zubrinic, Zupanovic) in the differentiable case, and related to the box dimension of the orbit. Here, we generalize these results to non-differentiable cases introducing a new notion of critical Minkowski order. We study the space of functions having a development in a Chebyshev scale and use multiplicity with respect to this space of functions. With the new definition, we recover the relationship between multiplicity o…

Critical Minkowski orderDynamical Systems (math.DS)Fixed pointsymbols.namesakeMinkowski spaceFOS: MathematicsCyclicityDifferentiable functionHomoclinic orbitlimit cycles; multiplicity; cyclicity; Chebyshev scale; Critical Minkowski order; box dimension; homoclinic loopMathematics - Dynamical SystemsAbelian groupPoincaré mapMathematicsBox dimensionApplied MathematicsMathematical analysisMultiplicity (mathematics)Limit cyclesMultiplicityPoincaré conjecturesymbols37G15 34C05 28A75 34C10Homoclinic loopAnalysisChebyshev scaleJournal of Differential Equations
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Infinite orbit depth and length of Melnikov functions

2019

Abstract In this paper we study polynomial Hamiltonian systems d F = 0 in the plane and their small perturbations: d F + ϵ ω = 0 . The first nonzero Melnikov function M μ = M μ ( F , γ , ω ) of the Poincare map along a loop γ of d F = 0 is given by an iterated integral [3] . In [7] , we bounded the length of the iterated integral M μ by a geometric number k = k ( F , γ ) which we call orbit depth. We conjectured that the bound is optimal. Here, we give a simple example of a Hamiltonian system F and its orbit γ having infinite orbit depth. If our conjecture is true, for this example there should exist deformations d F + ϵ ω with arbitrary high length first nonzero Melnikov function M μ along…

PolynomialDynamical Systems (math.DS)Iterated integrals01 natural sciencesHamiltonian system03 medical and health sciences0302 clinical medicineFOS: MathematicsCenter problem030212 general & internal medicine0101 mathematicsMathematics - Dynamical Systems[MATH]Mathematics [math]Mathematical PhysicsMathematical physicsPoincaré mapPhysicsConjecturePlane (geometry)Applied Mathematics010102 general mathematicsMSC : primary 34C07 ; secondary 34C05 ; 34C08Loop (topology)Bounded functionMAPOrbit (control theory)Analysis34C07 34C05 34C08
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Some Applications of the Poincaré-Bendixson Theorem

2021

We consider a C 1 vector field X defined on an open subset U of the plane, with compact closure. If X has no singular points and if U is simply connected, a weak version of the Poincaré-Bendixson Theorem says that the limit sets of X in U are empty but that one can defined non empty extended limit sets contained into the boundary of U. We give an elementary proof of this result, independent of the classical Poincaré-Bendixson Theorem. A trapping triangle T based at p, for a C 1 vector field X defined on an open subset U of the plane, is a topological triangle with a corner at a point p located on the boundary ∂U and a good control of the tranversality of X along the sides. The principal app…

2010 Mathematics Subject Classification. Primary: 34C05trapping triangles[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]separatrix[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Secondary: 34A26 weak Poincaré-Bendixson Theoremextended limit sets[MATH] Mathematics [math][MATH]Mathematics [math]
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