Title: Large Phenomena beyond all orders and bifurcation of reversible homoclinic connections. Applications to water waves. Speaker: Eric Lombardi, INLN, Nice In many physical problems one can construct ``solutions'' in term of power series of a small parameter $\epsilon$ which reads $ Y(t,\epsilon) = \sum\limits_{n= 0}^k \epsilon^n Y_n(t) + o(\epsilon^k).$ In some cases, this power series is defined at any order but it diverges. This divergence may express that the system has a solution for which such an expansion misses some exponentially small term like $e^{-1/\epsilon^2} Z(t)$. {\em Such a term is said to lie beyond any algebraic orders}. This kind of phenomena typically occurs for physical problems governed by reversible vector fields near resonances because of the degeneracy induced by the symmetry and the resonance. Such problems, in which these very small terms have great practical interest, are known in many branches of science including dendritic crystals growth, quantum tunneling, KAM theory, theory of water-waves (which was our original motivation for this work) and others. A careful study of these problem reveals that in most of the cases, the exponentially small terms come from {\em oscillatory integrals}. To study such problems, we have developed a general method to obtain an exponentially small equivalent of oscillatory integrals involving solutions of {\em nonlinear differential equations}. The method is based on a very precise description of the holomorphic continuation of the solutions of the perturbed equation and in particular of their behavior near the complex singularities of the solutions of the unperturbed system. The method that we use to build step by step the holomorphic continuation of the solutions is a rigorous version for this problem of the formal theory of Matching Asymptotic Expansions (M.A.E.). In particular, the construction of the holomorphic continuation of the solutions near the singularities is based on the study of an ``inner system'' which is well known in the theory of M.A.E. and which appears to be the relevant part of the equation near the singularities. This method enables us to study the problem of the persistence of homoclinic connections to 0 for the one parameter families $V(.,\mu)$ of reversible vector fields which admit at the origin a $0^2i\omega$ resonance, i.e. vector fields for which the origin is a fixed point and for which $0$ is a double non semi simple eigenvalues and $\pm i\omega$ are simple eigenvalues of the differential at the origin $DV_u(0,0)$. This problem cannot be solved by a direct Melnikov approach since the Melnikov function is given by an oscillatory integral and is exponentially small. Our ``Exponential tools'' enable us to prove [2] that generically, vector fields admitting at 0 a $0^{2}i\omega$ resonance at the origin do not admit any homoclinic connection to 0, whereas we proved in [1] that they always admit homoclinic connections to exponentially small periodic orbits. One example of such a vector field in infinite dimensions occurs when describing the irrotational flow of an inviscid fluid layer under the influence of gravity and small surface tension (Bond number $b<1/3$) for a Froude number $F$ close to $1$. In this context a homoclinic connection to 0 would be called a solitary wave. We have also developed a general method to obtain an exponentially small equivalent of bi-oscillatory integrals. In this case, the interaction between the two frequencies, makes the study more intricate and a partial complexification of time is necessary. This last method enables to study the $(i\omega_0)^2 i\omega_1$ resonance, i.e. one parameter families $V(\cdot, \mu)$ of reversible vector fields for which $\pm i \omega_0$ are a double non semi simple eigenvalues and $\pm i\omega_1$ are simple eigenvalues of the differential at the origin $DV_u(0,0)$. Such a resonance occurs for water waves when studying several layers problems and for chains of coupled nonlinear oscillators. [1] Lombardi E. Homoclinic orbits to exponentially small periodic orbits for a class of reversible systems. Application to water waves. {\em Arch. Rational Mech. Anal.}, {\bf 137}:p. 227-304, (1997). [2] Lombardi E. Oscillatory integrals and phenomena beyond any algebraic order; with applications to homoclinic orbits in reversible systems. Book in preparation.