234 research outputs found

    Sharp estimates on the first eigenvalue of the p-Laplacian with negative Ricci lower bound

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    We complete the picture of sharp eigenvalue estimates for the p-Laplacian on a compact manifold by providing sharp estimates on the first nonzero eigenvalue of the nonlinear operator Δp\Delta_p when the Ricci curvature is bounded from below by a negative constant. We assume that the boundary of the manifold is convex, and put Neumann boundary conditions on it. The proof is based on a refined gradient comparison technique and a careful analysis of the underlying model spaces.Comment: Sign mistake fixed in the proof of the gradient comparison theorem (theorem 5.1 pag 10), and some minor improvements aroun

    Z_2-Bi-Gradings, Majorana Modules and the Standard Model Action

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    The action functional of the Standard Model of particle physics is intimately related to a specific class of first order differential operators called Dirac operators of Pauli type ("Pauli-Dirac operators"). The aim of this article is to carefully analyze the geometrical structure of this class of Dirac operators on the basis of real Dirac operators of simple type. On the basis of simple type Dirac operators, it is shown how the Standard Model action (STM action) may be viewed as generalizing the Einstein-Hilbert action in a similar way the Einstein-Hilbert action is generalized by a cosmological constant. Furthermore, we demonstrate how the geometrical scheme presented allows to naturally incorporate also Majorana mass terms within the Standard Model. For reasons of consistency these Majorana mass terms are shown to dynamically contribute to the Einstein-Hilbert action by a "true" cosmological constant. Due to its specific form, this cosmological constant can be very small. Nonetheless, this cosmological constant may provide a significant contribution to dark matter/energy. In the geometrical description presented this possibility arises from a subtle interplay between Dirac and Majorana masses

    Some remarks on the isoperimetric problem for the higher eigenvalues of the Robin and Wentzell Laplacians

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    We consider the problem of minimising the kkth eigenvalue, k2k \geq 2, of the (pp-)Laplacian with Robin boundary conditions with respect to all domains in RN\mathbb{R}^N of given volume MM. When k=2k=2, we prove that the second eigenvalue of the pp-Laplacian is minimised by the domain consisting of the disjoint union of two balls of equal volume, and that this is the unique domain with this property. For p=2p=2 and k3k \geq 3, we prove that in many cases a minimiser cannot be independent of the value of the constant α\alpha in the boundary condition, or equivalently of the volume MM. We obtain similar results for the Laplacian with generalised Wentzell boundary conditions Δu+βuν+γu=0\Delta u + \beta \frac{\partial u}{\partial \nu} + \gamma u = 0.Comment: 16 page

    The heart of a convex body

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    We investigate some basic properties of the {\it heart} (K)\heartsuit(\mathcal{K}) of a convex set K.\mathcal{K}. It is a subset of K,\mathcal{K}, whose definition is based on mirror reflections of euclidean space, and is a non-local object. The main motivation of our interest for (K)\heartsuit(\mathcal{K}) is that this gives an estimate of the location of the hot spot in a convex heat conductor with boundary temperature grounded at zero. Here, we investigate on the relation between (K)\heartsuit(\mathcal{K}) and the mirror symmetries of K;\mathcal{K}; we show that (K)\heartsuit(\mathcal{K}) contains many (geometrically and phisically) relevant points of K;\mathcal{K}; we prove a simple geometrical lower estimate for the diameter of (K);\heartsuit(\mathcal{K}); we also prove an upper estimate for the area of (K),\heartsuit(\mathcal{K}), when K\mathcal{K} is a triangle.Comment: 15 pages, 3 figures. appears as "Geometric Properties for Parabolic and Elliptic PDE's", Springer INdAM Series Volume 2, 2013, pp 49-6

    A remark on an overdetermined problem in Riemannian Geometry

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    Let (M,g)(M,g) be a Riemannian manifold with a distinguished point OO and assume that the geodesic distance dd from OO is an isoparametric function. Let ΩM\Omega\subset M be a bounded domain, with OΩO \in \Omega, and consider the problem Δpu=1\Delta_p u = -1 in Ω\Omega with u=0u=0 on Ω\partial \Omega, where Δp\Delta_p is the pp-Laplacian of gg. We prove that if the normal derivative νu\partial_{\nu}u of uu along the boundary of Ω\Omega is a function of dd satisfying suitable conditions, then Ω\Omega must be a geodesic ball. In particular, our result applies to open balls of Rn\mathbb{R}^n equipped with a rotationally symmetric metric of the form g=dt2+ρ2(t)gSg=dt^2+\rho^2(t)\,g_S, where gSg_S is the standard metric of the sphere.Comment: 8 pages. This paper has been written for possible publication in a special volume dedicated to the conference "Geometric Properties for Parabolic and Elliptic PDE's. 4th Italian-Japanese Workshop", organized in Palinuro in May 201

    Second-order L2L^2-regularity in nonlinear elliptic problems

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    A second-order regularity theory is developed for solutions to a class of quasilinear elliptic equations in divergence form, including the pp-Laplace equation, with merely square-integrable right-hand side. Our results amount to the existence and square integrability of the weak derivatives of the nonlinear expression of the gradient under the divergence operator. This provides a nonlinear counterpart of the classical L2L^2-coercivity theory for linear problems, which is missing in the existing literature. Both local and global estimates are established. The latter apply to solutions to either Dirichlet or Neumann boundary value problems. Minimal regularity on the boundary of the domain is required. If the domain is convex, no regularity of its boundary is needed at all

    On the regularity up to the boundary for certain nonlinear elliptic systems

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    We consider a class of nonlinear elliptic systems and we prove regularity up to the boundary for second order derivatives. In the proof we trace carefully the dependence on the various parameters of the problem, in order to establish, in a further work, results for more general systems
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