Geodesic

Sommaire du Fascicule no. 1

Homoclinic and period-doubling bifurcations for damped systems
p. 1-25
Geodesics on product lorentzian manifolds
p. 27-60
Connectivity properties of the range of a weak diffeomorphism
p. 61-73
Topological solutions in the self-dual Chern-Simons theory : existence and approximation
p. 75-97
Some constancy results for nematic liquid crystals and harmonic maps
p. 99-115

Sommaire du Fascicule no. 2

Microscopic structure of shocks in one conservation laws
p. 119-153
Asymptotic behaviour of solutions and their derivatives, for semilinear elliptic problems with blowup on the boundary
p. 155-171
Non-uniqueness of solutions of nonlinear heat equations of fast diffusion type
p. 173-200
Second order nonpersistence of the sine Gordon breather under an exceptional perturbation
p. 201-239

Sommaire du Fascicule no. 3

Vortices for a variational problem related to superconductivity
p. 243-303
Unicité et minimalité des solutions d'une équation de Ginzburg-Landau
p. 305-318
A note on compactness-type properties with respect to Lorentz norms of bounded subsets of a Sobolev Space
p. 319-337
Nonlinear instability of double-humped equilibria
p. 339-352

Sommaire du Fascicule no. 4

Regularity of solutions for some problems of mathematical physics
p. 355-413
A note on weak approximation of minors
p. 415-424
Asymptotic behaviour of solutions to the Korteweg-de Vries-Burgers system
p. 425-457
Normal form and global solutions for the Klein-Gordon-Zakharov equations
p. 459-503

Sommaire du Fascicule no. 5

Nonlinear oblique boundary value problems for hessian equations in two dimensions
p. 507-575
Estimates for solutions of nonlinear variational inequalities
p. 577-597
Solutions of Ginzburg-Landau equations and critical points of the renormalized energy
p. 599-622

Sommaire du Fascicule no. 6

A solution to the bidimensional global asymptotic stability conjecture
p. 627-671
Gevrey regularizing effect for the (generalized) Korteweg-de Vries equation and nonlinear Schrödinger equations
p. 673-725
Sur l’équation générale u t =a(.,u,ϕ(.,u) x ) x +v dans L 1 : II. Le problème d’évolution
p. 727-761