Jean-Pierre Gossez
Université libre de Bruxelles
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Transactions of the American Mathematical Society | 1974
Jean-Pierre Gossez
Variational boundary value problems for quasilinear elliptic systems in divergence form are studied in the case where the nonlinearities are nonpolynomial. Monotonicity methods are used to derive several existence theorems which generalize the basic results of Browder and Leray-Lions. Some features of the mappings of monotone type which arise here are that they act in nonreflexive Banach spaces, that they are unbounded and not everywhere defined, and that their inverse is also unbounded and not everywhere defined.
Journal of Functional Analysis | 2003
Djairo G. de Figueiredo; Jean-Pierre Gossez; Pedro Ubilla
In this paper the usual notions of superlinearity and sublinearity for semilinear problems like _Du ¼ f ðx; uÞ are given a local form and extended to indefinite nonlinearities. Here f ðx; sÞ is allowed to change sign or to vanish for s near zero as well as for s near infinity. Some of the well-known results of Ambrosetti–Bre′zis–Cerami are partially extended to this context.
Communications in Partial Differential Equations | 1992
Djairo G. de Figueiredo; Jean-Pierre Gossez
In this paper, we show that the strict monotonicity of the eigenvalues of an uniformly elliptic operator of second order is equivalent to a unique continuation property.
Journal of Differential Equations | 1991
Jean-Pierre Gossez; Pierpaolo Omari
The nonlinearity g in (1.1) is a continuous function from R to R and the forcing term h is taken in L”(O,27r). Nonresonance means that (1.1) admits at least one solution x for any given h. Integrating Eq. (1.1) over a period, one immediately sees that a necessary condition for nonresonance is that the function g be unbounded from above and from below on R. It will appear later (cf. (1.6)) that this unboundedness can be looked at as a condition relating the behaviour at infinity of the nonlinearity g with respect to the first eigenvalue 1, = 0 of the associated linear problem: -xf’= Ax in [0, 27r], x(0) = x(27r), x’(0) = x1(271). (1.2)
Journal of the European Mathematical Society | 2006
Djairo G. de Figueiredo; Jean-Pierre Gossez; Pedro Ubilla
In this paper we study the existence, nonexistence and multiplicity of positive solutions for the family of problems
Journal of Differential Equations | 1978
Djairo Guedes de Figueiredo; Jean-Pierre Gossez
-\Delta u = f_\lambda (x,u)
Nonlinear Analysis-theory Methods & Applications | 2002
T. Godoy; Jean-Pierre Gossez; S. Paczka
,
Annales De L Institut Henri Poincare-analyse Non Lineaire | 2002
Margarita Arias; Juan Campos; Mabel Cuesta; Jean-Pierre Gossez
u \in H^1_0(\Omega)
Proceedings of the American Mathematical Society | 1972
Jean-Pierre Gossez
, where
Comptes Rendus De L Academie Des Sciences Serie I-mathematique | 2000
Mabel Cuesta; Djairo G. de Figueiredo; Jean-Pierre Gossez
\Omega