Bifurcations without parameters: some ODE and PDE examples

dc.creatorFiedler, Bernold
dc.creatorLiebscher, Stefan
dc.date2003-04-28
dc.date.accessioned2026-07-07T04:57:31Z
dc.date.available2026-07-07T04:57:31Z
dc.descriptionStandard bifurcation theory is concerned with families of vector fields $dx/dt = f(x,λ)$, $x \in \R^n$, involving one or several constant real parameters $λ$. Viewed as a differential equation for the pair $(x,λ)$, we observe a foliation of the total phase space by constant $λ$. Frequently, the presence of a trivial stationary solution $x=0$ is also imposed: $0 = f(0,λ)$. Bifurcation without parameters, in contrast, discards the foliation by a constant parameter $λ$. Instead, we consider systems $dx/dt = f(x,y), dy/dt = g(x,y)$. Standard bifurcation theory then corresponds to the special case $y=λ, g=0$. To preserve only the trivial solution $x=0$, instead, we only require $0 = f(0,y) = g(0,y)$ for all $y$. A rich dynamic phenomenology arises, when normal hyperbolicity of the trivial stationary manifold $x=0$ fails, due to zero or purely imaginary eigenvalues of the Jacobian $f_x(0,y)$. Specifically, we address the cases of failure of normal hyperbolicity due to a simple eigenvalue zero, a simple purely imaginary pair (Hopf bifurcation without parameters), a double eigenvalue zero (Takens-Bogdanov bifurcation without parameters), and due to a double eigenvalue zero with additional time reversal symmetries. The results are joint work with Andrei Afendikov, James C. Alexander, and Stefan Liebscher.
dc.identifierhttps://arxiv.org/abs/math/0304453
dc.identifierhttp://arxiv.org/abs/math/0304453
dc.identifierProceedings of the ICM, Beijing 2002, vol. 3, 305--316
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/67285
dc.subjectDynamical Systems
dc.subject34C23, 34C29, 34C37
dc.titleBifurcations without parameters: some ODE and PDE examples
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