375 research outputs found
Resonant Bifurcations
We consider dynamical systems depending on one or more real parameters, and
assuming that, for some ``critical'' value of the parameters, the eigenvalues
of the linear part are resonant, we discuss the existence -- under suitable
hypotheses -- of a general class of bifurcating solutions in correspondence to
this resonance. These bifurcating solutions include, as particular cases, the
usual stationary and Hopf bifurcations. The main idea is to transform the given
dynamical system into normal form (in the sense of Poincar\'e-Dulac), and to
impose that the normalizing transformation is convergent, using the convergence
conditions in the form given by A. Bruno. Some specially interesting
situations, including the cases of multiple-periodic solutions, and of
degenerate eigenvalues in the presence of symmetry, are also discussed with
some detail.Comment: PlainTeX, no figure
Convergent Normal Forms of Symmetric Dynamical Systems
It is shown that the presence of Lie-point-symmetries of (non-Hamiltonian)
dynamical systems can ensure the convergence of the coordinate transformations
which take the dynamical sytem (or vector field) into Poincar\'e-Dulac normal
form.Comment: 11 pag., Plain Te
On the convergence of normalizing transformations in the presence of symmetries
It is shown that, under suitable conditions, involving in particular the
existence of analytic constants of motion, the presence of Lie point symmetries
can ensure the convergence of the transformation taking a vector field (or
dynamical system) into normal form.Comment: 14 pag, Plain Te
Twisted symmetries and integrable systems
Symmetry properties are at the basis of integrability. In recent years, it
appeared that so called "twisted symmetries" are as effective as standard
symmetries in many respects (integrating ODEs, finding special solutions to
PDEs). Here we discuss how twisted symmetries can be used to detect
integrability of Lagrangian systems which are not integrable via standard
symmetries
Convergence of normal form transformations: The role of symmetries
We discuss the convergence problem for coordinate transformations which take
a given vector field into Poincar\'e-Dulac normal form. We show that the
presence of linear or nonlinear Lie point symmetries can guaranteee convergence
of these normalizing transformations, in a number of scenarios. As an
application, we consider a class of bifurcation problems.Comment: 20 pages, no figure
An approach to Mel'nikov theory in celestial mechanics
Using a completely analytic procedure - based on a suitable extension of a
classical method - we discuss an approach to the Poincar\'e-Mel'nikov theory,
which can be conveniently applied also to the case of non-hyperbolic critical
points, and even if the critical point is located at the infinity. In this
paper, we concentrate our attention on the latter case, and precisely on
problems described by Kepler-like potentials in one or two degrees of freedom,
in the presence of general time-dependent perturbations. We show that the
appearance of chaos (possibly including Arnol'd diffusion) can be proved quite
easily and in a direct way, without resorting to singular coordinate
transformations, such as the McGehee or blowing-up transformations. Natural
examples are provided by the classical Gyld\'en problem, originally proposed in
celestial mechanics, but also of interest in different fields, and by the
general 3-body problem in classical mechanics.Comment: LaTeX, no figure
Side conditions for ordinary differential equations
We specialize Olver's and Rosenau's side condition heuristics for the
determination of particular invariant sets of ordinary differential equations.
It turns out that side conditions of so-called LaSalle type are of special
interest. Moreover we put side condition properties of symmetric and partially
symmetric equations in a wider context. In the final section we present an
application to parameter-dependent systems, in particular to quasi-steady state
for chemical reactions.Comment: To appear in J. of Lie Theor
- …