Abstract:In this work we develop a systematic geometric approach to study fully nonlinear elliptic equations with singular absorption terms as well as their related free boundary problems. The magnitude of the singularity is measured by a negative parameter (γ − 1), for 0 < γ < 1, which reflects on lack of smoothness for an existing solution along the singular interface between its positive and zero phases. We establish existence as well sharp regularity properties of solutions. We further prove that minimal solutions … Show more
“…This is not an obstacle problem explicitly but the solutions are automatically constrained above zero, thus it is equivalent to the problem with the constraint u ≥ ψ ≡ 0 (flat obstacle problem). This problem is one of important interface models and has been generalized variously (for example, see [25] generalizing the first term, [3] the second term, or their references). Especially, Yamaura [33] considered a non-linearized case, namely the case that the first term is replaced to the area functional.…”
Section: Viewpoint Of Energies and Settingsmentioning
A free boundary problem arising from materials science is studied in the one-dimensional case. The problem studied here is an obstacle problem for the non-convex energy consisting of a bending energy, tension and an adhesion energy. If the bending energy, which is a higher order term, is deleted then "edge" singularities of the solutions (surfaces) may occur at the free boundary as Alt-Caffarelli type variational problems. The main result of this paper is to give a singular limit of the energy utilizing the notion of Γ-convergence, when the bending energy can be regarded as a perturbation. This singular limit energy only depends on the state of surfaces at the free boundary as seen in singular perturbations for phase transition models.2010 Mathematics Subject Classification. 35B25, and 35R35.
“…This is not an obstacle problem explicitly but the solutions are automatically constrained above zero, thus it is equivalent to the problem with the constraint u ≥ ψ ≡ 0 (flat obstacle problem). This problem is one of important interface models and has been generalized variously (for example, see [25] generalizing the first term, [3] the second term, or their references). Especially, Yamaura [33] considered a non-linearized case, namely the case that the first term is replaced to the area functional.…”
Section: Viewpoint Of Energies and Settingsmentioning
A free boundary problem arising from materials science is studied in the one-dimensional case. The problem studied here is an obstacle problem for the non-convex energy consisting of a bending energy, tension and an adhesion energy. If the bending energy, which is a higher order term, is deleted then "edge" singularities of the solutions (surfaces) may occur at the free boundary as Alt-Caffarelli type variational problems. The main result of this paper is to give a singular limit of the energy utilizing the notion of Γ-convergence, when the bending energy can be regarded as a perturbation. This singular limit energy only depends on the state of surfaces at the free boundary as seen in singular perturbations for phase transition models.2010 Mathematics Subject Classification. 35B25, and 35R35.
“…This notion also appears naturally in the study of free boundary problems governed by fully nonlinear operators, see [14,3]. The idea is that the family F µ (M) := µF(µ −1 M) forms a path of uniform elliptic operators (each F µ is elliptic with the same ellipticity constants as F), jointing F and F ⋆ .…”
“…Similarly, u is a viscosity supersolution to (1) if whenever one touches the graph of u from below by a smooth function φ at y 0 ∈ B 1 , there holds…”
We establish sharp W 2,p regularity estimates for viscosity solutions of fully nonlinear elliptic equations under minimal, asymptotic assumptions on the governing operator F. By means of geometric tangential methods, we show that if the recession of the operator F -formally given bywith appropriate universal estimates. Our result extends to operators with variable coefficients and in this setting they are new even under convexity of the frozen coefficient operator, M → F(x 0 , M), as oscillation is measured only at the recession level. The methods further yield BMO regularity of the hessian, provided the source lies in that space. As a final application, we establish the density of W 2,p solutions within the class of all continuous viscosity solutions, for generic fully nonlinear operators F. This result gives an alternative tool for treating common issues often faced in the theory of viscosity solutions.
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