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Overstability and resonance

Augustin Fruchard, Reinhard Schäfke (2003)

Annales de l’institut Fourier

We consider a singularity perturbed nonlinear differential equation ε u ' = f ( x ) u + + ε P ( x , u , ε ) which we suppose real analytic for x near some interval [ a , b ] and small | u | , | ε | . We furthermore suppose that 0 is a turning point, namely that x f ( x ) is positive if x 0 . We prove that the existence of nicely behaved (as ϵ 0 ) local (at x = 0 ) or global, real analytic or C solutions is equivalent to the existence of a formal series solution u n ( x ) ε n with u n analytic at x = 0 . The main tool of a proof is a new “principle of analytic continuation” for such “overstable” solutions....

Painlevé equations and complex reflections

Philip Boalch (2003)

Annales de l’institut Fourier

We will explain how some new algebraic solutions of the sixth Painlevé equation arise from complex reflection groups, thereby extending some results of Hitchin and Dubrovin-- Mazzocco for real reflection groups. The problem of finding explicit formulae for these solutions will be addressed elsewhere.

Periodic integrals and tautological systems

Bong H. Lian, Ruifang Song, Shing-Tung Yau (2013)

Journal of the European Mathematical Society

We study period integrals of CY hypersurfaces in a partial flag variety. We construct a regular holonomic system of differential equations which govern the period integrals. By means of representation theory, a set of generators of the system can be described explicitly. The results are also generalized to CY complete intersections. The construction of these new systems of differential equations has lead us to the notion of a tautological system.

Perturbation singulière en dimension trois : canards en un point pseudo-singulier nœud

Éric Benoît (2001)

Bulletin de la Société Mathématique de France

On étudie les systèmes différentiels singulièrement perturbés de dimension 3 du type { x ˙ = f ( x , y , z , ε ) , y ˙ = g ( x , y , z , ε ) , ε z ˙ = h ( x , y , z , ε ) , f , g , h sont analytiques quelconques. Les travaux antérieurs étudiaient les points réguliers où la surface lente h = 0 est transverse au champ rapide vertical. C’est le domaine d’application du théorème de Tikhonov. Dans d’autres travaux antérieurs, on étudiait les singularités de certains types : plis et fronces de la surface lente, ainsi que certaines singularités plus compliquées, analogues aux points tournants...

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