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  • Articles  (48)
  • bifurcation  (48)
  • Springer  (48)
  • American Chemical Society (ACS)
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  • 1995-1999  (46)
  • 1980-1984  (2)
  • Mathematics  (48)
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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Journal of dynamics and differential equations 11 (1999), S. 515-555 
    ISSN: 1572-9222
    Keywords: Traveling wave ; eigenvalue problem ; bifurcation ; topological method
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract Consideration is devoted to traveling N-front wave solutions of the FitzHugh–Nagumo equations of the bistable type. Especially, stability of the N-front wave is proven. In the proof, the eigenvalue problem for the N-front wave bifurcating from coexisting simple front and back waves is regarded as a bifurcation problem for projectivised eigenvalue equations, and a topological index is employed to detect eigenvalues.
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Journal of dynamics and differential equations 8 (1996), S. 549-572 
    ISSN: 1572-9222
    Keywords: homoclinic obit ; bifurcation ; Conley index
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract We study bifurcations, calledN-homoclinic bifurcations, which produce homoclinic orbits roundingN times (N⩾2) in some tubular neighborhood of original homoclinic orbit. A family of vector fields undergoes such a bifurcation when it is a perturbation of a vector field with a homoclinic orbit.N-Homoclinic bifurcations are divided into two cases; one is that the linearization at the equilibrium has only real principal eigenvalues, and the other is that it has complex principal eigenvalues. We treat the former case, espcially that linearization has only one unstable eigenvalue. As main tools we use a topological method, namely, Conley index theory, which enables us to treat more degenerate cases than those studied by analytical methods.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Journal of dynamics and differential equations 11 (1999), S. 671-709 
    ISSN: 1572-9222
    Keywords: Homoclinic orbits ; singular perturbations ; bifurcation ; FitzHugh–Nagumo system
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract Homoclinic orbits in the fast dynamics of singular perturbation problems are usually analyzed by a combination of Fenichel's invariant manifold theory with general transversality arguments (see Ref. 29 and the Exchange Lemma in Ref. 16). In this paper an alternative direct approach is developed which uses a two-time scaling and a contraction argument in exponentially weighted spaces. Homoclinic orbits with one last transition are treated and it is shown how ε-expansions can be extracted rigorously from this approach. The result is applied to a singularity perturbed Bogdanov point in the FitzHugh–Nagumo system.
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Journal of dynamics and differential equations 11 (1999), S. 129-208 
    ISSN: 1572-9222
    Keywords: Reversible systems ; bifurcation ; normal forms ; oscillatory integrals ; exponential splitting
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract The dynamics of an analytic reversible vector field $$V$$ (X,μ) is studied in $$\mathbb{R}^4 $$ with one real parameter μ close to 0; X=0 is a fixed point. The differential Dx $$V$$ (0,0) generates an “oscillatory” dynamics with a frequency of order 1—due to two simple, opposite eigenvalues lying on the imaginary axis—and it also generates a “slow” dynamics which changes from a hyperbolic type—eigenvalues are $$ \pm \sqrt { - \mu } $$ —to an elliptic type—eigenvalues are $$ \pm {\text{ }}i{\text{ }}\sqrt \mu $$ —as μ passes trough 0. The existence of reversible homoclinic connections to periodic orbits is known for such vector fields. In this paper we study a particular subclass of such vector fields, obtained by small reversible perturbations of the normal form. We give an explicit condition on the perturbation, generically satisfied, which prevents the existence of a homoclinic connections to 0 for the perturbed system. The normal form system of any order admits a reversible homoclinic connection to 0, which then does not survive under perturbation of higher order. It will be seen that normal form essentially decouples the hyperbolic and elliptic part of the linearization to any chosen algebraic order. However, this decoupling does not persist arbitrary reversible perturbation, which finally causes the appearance of small amplitude oscillations.
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Journal of dynamics and differential equations 8 (1996), S. 221-279 
    ISSN: 1572-9222
    Keywords: Homoclinic orbits ; Hamiltonian systems ; bifurcation ; dynamical systems ; water waves ; elastic struts
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract This is a further study of the set of homoclinic solutions (i.e., nonzero solutions asymptotic to 0 as ¦x¦→∞) of the reversible Hamiltonian systemu iv +Pu″ +u−u 2=0. The present contribution is in three parts. First, rigorously for P≤ −2, it is proved that there is a unique (up to translation) homoclinic solution of the above system, that solution is even, and on the zero-energy surface its orbit coincides with the transverse intersection of the global stable and unstable manifolds. WhenP=−2 the origin is a node on its local stable and unstable manifolds, and whenP∈(−2,2) it is a focus. Therefore we can infer, rigorously, from the discovery by Devaney of a Smale horseshoe in the dynamics on the zero energy set, there are infinitely many distinct infinite families of homoclinic solutions forP∈(−2, −2+ε) for someε〉0. Buffoni has shown globally that there are infinitely many homoclinic solutions for allP∈(−2,0], based on a different approach due to Champneys and Toland. Second, numerically, the development of the set of symmetric homoclinic solutions is monitored asP increases fromP=−2. It is observed that two branches extend fromP=−2 toP=+2 where their amplitudes are found to converge to 0 asP ↗ 2. All other symmetric solution branches are in the form of closed loops with a turning point betweenP=−2 andP=+2. Numerically it is observed that each such turning point is accompanied by, though not coincident with, the bifurcation of a branch of nonsymmetrical homoclinic orbits, which can, in turn, be followed back toP=−2. Finally, heuristic explanations of the numerically observed phenomena are offered in the language of geometric dynamical systems theory. One idea involves a natural ordering of homoclinic orbits on the stable and unstable manifolds, given by the Horseshoe dynamics, and goes some way to accounting for the observed order (in terms ofP-values) of the occurrence of turning points. The near-coincidence of turning and asymmetric bifurcation points is explained in terms of the nontransversality of the intersection of the stable and unstable manifolds in the zero energy set on the one hand, and the nontransversality of the intersection of the same manifolds with the symmetric section in ℝ4 on the other. Some conjectures based on present understanding are recorded.
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  • 6
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    Electronic Resource
    Springer
    Georgian mathematical journal 4 (1997), S. 567-578 
    ISSN: 1572-9176
    Keywords: Flow ; bifurcation ; perturbation ; axisymmetric flow ; permeable cylinders
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract Sufficient conditions are found for the bifurcation of flow of a viscous heat-conducting fluid between two rotating permeable cylinders.
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  • 7
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    Springer
    Applications of mathematics 42 (1997), S. 421-449 
    ISSN: 1572-9109
    Keywords: reaction-diffusion systems ; variational inequalities ; inclusions ; bifurcation ; stationary solutions ; spatial patterns
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract We consider a reaction-diffusion system of the activator-inhibitor type with boundary conditions given by inclusions. We show that there exists a bifurcation point at which stationary but spatially nonconstant solutions (spatial patterns) bifurcate from the branch of trivial solutions. This bifurcation point lies in the domain of stability of the trivial solution to the same system with Dirichlet and Neumann boundary conditions, where a bifurcation of this classical problem is excluded.
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  • 8
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    Springer
    Czechoslovak mathematical journal 47 (1997), S. 469-486 
    ISSN: 1572-9141
    Keywords: reaction-diffusion systems ; unilateral conditions ; bifurcation ; quasivariational inequalities ; spatial patterns
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract Reaction-diffusion systems are studied under the assumptions guaranteeing diffusion driven instability and arising of spatial patterns. A stabilizing influence of unilateral conditions given by quasivariational inequalities to this effect is described.
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  • 9
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    Springer
    Czechoslovak mathematical journal 49 (1999), S. 449-474 
    ISSN: 1572-9141
    Keywords: bifurcation ; periodic solutions ; variational inequality ; differential inequality ; finite dimensional space ; Alexander-Yorke theorem
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics
    Notes: Abstract Variational inequalities $$\begin{gathered} U(t) \in K, \hfill \\ (\dot U(t) - B_\lambda U(t) - G(\lambda ,U(t)),\;\;Z - U(t)) \geqslant 0 for all Z \in K, a .a . t \in (0,T) \hfill \\ \end{gathered} $$ are studied, where K is a closed convex cone in $${\mathbb{R}}^{\kappa } $$ , κ ≥ 3, B λ is a κ × κ matrix, G is a small perturbation, λ a real parameter. The assumptions guaranteeing a Hopf bifurcation at some λ0 for the corresponding equation are considered and it is proved that then, in some situations, also a bifurcation of periodic solutions to our inequality occurs at some λI ≠ λ0. Bifurcating solutions are obtained by the limiting process along branches of solutions to penalty problems starting at λ0 constructed on the basis of the Alexander-Yorke theorem as global bifurcation branches of a certain enlarged system.
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  • 10
    Electronic Resource
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    Springer
    Zeitschrift für angewandte Mathematik und Physik 47 (1996), S. 567-590 
    ISSN: 1420-9039
    Keywords: 76E15 ; 76E30 ; Fluid dynamics ; convection ; bifurcation ; pattern formation
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Abstract Two immiscible liquids lie between parallel plates and are heated from below. The focus is on the case where the interfacial mode is strongly stabilized by surface tension and a suitable density stratification. A mechanism for a Hopf bifurcation is the competition between the least stable of the bulk modes in each fluid. The well known criterion for balancing the effective Rayleigh numbers in both fluids is augmented with a criterion for non-self-adjointness of the system, yielding a heuristic method for picking suitable fluids when Hopf modes are desired. The pattern formation problem in three dimensions is addressed for the case of doubly periodic solutions on a hexagonal lattice. Of the solutions with maximal symmetry, the travelling rolls are found to be stable.
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