International audienceIn this work, we consider germs of analytic singular vector elds in (C^3,0) with an isolated and doubly-resonant singularity of saddle-node type at the origin. Such vector elds come from irregular two-dimensional dierential systems with two opposite non-zero eigenvalues, and appear for instance when studying the irregular singularity at innity in Painlevé equations (P j) j=I,...,V for generic values of the parameters. Under suitable assumptions, we prove a theorem of analytic normalization over sectorial domains, analogous to the classical one due to Hukuhara-Kimura-Matuda for saddle-nodes in (C^2,0). We also prove that these maps are in fact the Gevrey-1 sums of the formal normalizing map, the existence of which has b...
We study the topology of the fibers of real analytic maps 'R POT.N'→'R POT.P', n>p, in a neighborhoo...
We present a geometric proof of the Poincaré-Dulac Normalization Theorem for analytic vector fields ...
The equation (z) over dot = e(i alpha)z + e(i phi)z\z\(2) + bz(-3) models a map near a Hopf bifurcat...
We consider germs of analytic singular vector fields in dimension three, called doubly-resonant sadd...
On considère des germes de champs de vecteurs holomorphes singuliers trimimensionnels, appelés noeud...
Nonlinear vector fields have two important types of singularities: the fixed points in phase space a...
International audienceBorel summable divergent series usually appear when studying solutions of anal...
The thesis is composed of a chapter of preliminaries and two articles on the theme ofunfolding of si...
This paper is concerned with the dynamics near an equilibrium point of reversible systems. For a lar...
A systematic construction of isomonodromic families of connections of rank two on the Riemarm sphere...
In this paper we study on ℝ3 a class of smoothly (C∞) finitely determined vector fields which admit ...
International audienceAmong all bifurcation behaviors of analytic parametric families of real planar...
We provide a unique normal form for rank two irregular connections on the Riemann sphere.In fact, we...
The investigation objects are the special points of the holomorphic vector fields on the complex pla...
The equation (z) over dot = e(i alpha)z + e(i phi)z\z\(2) + bz(-3) models a map near a Hopf bifurcat...
We study the topology of the fibers of real analytic maps 'R POT.N'→'R POT.P', n>p, in a neighborhoo...
We present a geometric proof of the Poincaré-Dulac Normalization Theorem for analytic vector fields ...
The equation (z) over dot = e(i alpha)z + e(i phi)z\z\(2) + bz(-3) models a map near a Hopf bifurcat...
We consider germs of analytic singular vector fields in dimension three, called doubly-resonant sadd...
On considère des germes de champs de vecteurs holomorphes singuliers trimimensionnels, appelés noeud...
Nonlinear vector fields have two important types of singularities: the fixed points in phase space a...
International audienceBorel summable divergent series usually appear when studying solutions of anal...
The thesis is composed of a chapter of preliminaries and two articles on the theme ofunfolding of si...
This paper is concerned with the dynamics near an equilibrium point of reversible systems. For a lar...
A systematic construction of isomonodromic families of connections of rank two on the Riemarm sphere...
In this paper we study on ℝ3 a class of smoothly (C∞) finitely determined vector fields which admit ...
International audienceAmong all bifurcation behaviors of analytic parametric families of real planar...
We provide a unique normal form for rank two irregular connections on the Riemann sphere.In fact, we...
The investigation objects are the special points of the holomorphic vector fields on the complex pla...
The equation (z) over dot = e(i alpha)z + e(i phi)z\z\(2) + bz(-3) models a map near a Hopf bifurcat...
We study the topology of the fibers of real analytic maps 'R POT.N'→'R POT.P', n>p, in a neighborhoo...
We present a geometric proof of the Poincaré-Dulac Normalization Theorem for analytic vector fields ...
The equation (z) over dot = e(i alpha)z + e(i phi)z\z\(2) + bz(-3) models a map near a Hopf bifurcat...