134 research outputs found

    A sharp inequality for Sobolev functions

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    Let N5N\geq 5, a>0a>0, Ω\Omega be a smooth bounded domain in RN\mathbb{R}^{N}, 2=2NN22^*=\frac{2N}{N-2}, 2#=2(N1)N22^\#=\frac{2(N-1)}{N-2} and u2=u22+au22||u||^2=|\nabla u|_{2}^2+a|u|_{2}^2. We prove there exists an α0>0\alpha_{0}>0 such that, for all uH1(Ω){0}u\in H^1(\Omega)\setminus\{0\}, S22Nu2u22(1+α0u2#2#uu22/2).\frac{S}{2^{\frac 2N}}\leq\frac{||u||^2}{|u|_{2^*}^2}\left(1+\alpha_{0}\frac{|u|_{2^\#}^{2^\#}}{||u||\cdot|u|_{2^*}^{2^*/2}}\right). This inequality implies Cherrier's inequality.Comment: 4 page

    A family of sharp inequalities for Sobolev functions

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    Let N5N\geq 5, Ω\Omega be a smooth bounded domain in RN\mathbb{R}^{N}, 2=2NN2{2^*}=\frac{2N}{N-2}, a>0a>0, S=inf{RNu2uL2(RN),uL2(RN),RNu2=1}S=\inf\left\{\left. \int_{\mathbb{R}^{N}}|\nabla u|^2\,\right|\,u\in L^{2^*}(\mathbb{R}^{N}), \nabla u\in L^2(\mathbb{R}^{N}), \int_{\mathbb{R}^{N}}|u|^{2^*}=1 \right\} and u2=u22+au22||u||^2=|\nabla u|_{2}^2+a|u|_{2}^2. We define 2=2NN1{2^\flat}= \frac{2N}{N-1}, 2#=2(N1)N2{2^\#}=\frac{2(N-1)}{N-2} and consider qq such that 2q2#{2^\flat}\leq q\leq{2^\#}. We also define s=2N+q2qs=2-N+\frac{q}{{2^*}-q} and t=2N212qt=\frac{2}{N-2}\cdot \frac{1}{{2^*}-q}. We prove that there exists an α0(q,a,Ω)>0\alpha_{0}(q,a,\Omega)>0 such that, for all uH1(Ω){0}u\in H^1(\Omega)\setminus\{0\}, S22Nu22u2+α0(uu22/2)suqqt,(I)q\frac{S}{2^{\frac 2N}}{|u|_{{2^*}}^2}\leq||u||^2+\alpha_{0} \left(\frac{||u||}{|u|_{{2^*}}^{2^*/2}}\right)^s|u|_{q}^{qt},\qquad{(I)_{q}} where the norms are over Ω\Omega. Inequality (I)2(I)_{{2^\flat}} is due to M. Zhu.Comment: 25 pages. arXiv admin note: text overlap with arXiv:1407.623

    Bifurcation curves of a logistic equation when the linear growth rate crosses a second eigenvalue

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    We construct the global bifurcation curves, solutions versus level of harvesting, for the steady states of a diffusive logistic equation on a bounded domain, under Dirichlet boundary conditions and other appropriate hypotheses, when aa, the linear growth rate of the population, is below λ2+δ\lambda_2+\delta. Here λ2\lambda_2 is the second eigenvalue of the Dirichlet Laplacian on the domain and δ>0\delta>0. Such curves have been obtained before, but only for aa in a right neighborhood of the first eigenvalue. Our analysis provides the exact number of solutions of the equation for aλ2a\leq\lambda_2 and new information on the number of solutions for a>λ2a>\lambda_2.Comment: This is an extended version of the published pape

    Convergence of a crystalline algorithm for the motion of a simple closed convex curve by weighted curvature

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    Motion by weighted mean curvature is a geometric evolution law for surfaces and represents steepest descent with respect to anisotropic surface energy. It has been proposed that this motion could be computed numerically by using a "crystalline" approximation to the surface energy in the evolution law. In this paper we prove the convergence of this numerical method for the case of simple closed convex curves in the plane.Comment: 14 pages, 3 figure

    On the Fu\v{c}ik spectrum of the wave operator and an asymptotically linear problem

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    We study generalized solutions of the nonlinear wave equation uttuss=au+bu+p(s,t,u),u_{tt}-u_{ss}=au^+-bu^-+p(s,t,u), with periodic conditions in tt and homogeneous Dirichlet conditions in ss, under the assumption that the ratio of the period to the length of the interval is two. When p0p\equiv 0 and λ\lambda is a nonzero eigenvalue of the wave operator, we give a proof of the existence of two families of curves (which may coincide) in the Fu\v{c}ik spectrum intersecting at (λ,λ)(\lambda,\lambda). This result is known for some classes of self-adjoint operators (which does not cover the situation we consider here), but in a smaller region than ours. Our approach is based on a dual variational formulation and is also applicable to other operators, such as the Laplacian. In addition, we prove an existence result for the nonhomogeneous situation, when the pair (a,b)(a,b) is not `between' the Fu\v{c}ik curves passing through (λ,λ)(0,0)(\lambda,\lambda)\neq(0,0) and pp is a continuous function, sublinear at infinity

    The shape of extremal functions for Poincar\'e-Sobolev-type inequalities in a ball

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    We study extremal functions for a family of Poincar\'e-Sobolev-type inequalities. These functions minimize, for subcritical or critical p2p\geq 2, the quotient u2/up{\|\nabla u\|_2}/{\|u\|_p} among all uH1(B){0}u \in H^1(B)\setminus\{0\} with Bu=0\int_{B}u=0. Here BB is the unit ball in RN\mathbb{R}^N. We show that the minimizers are axially symmetric with respect to a line passing through the origin. We also show that they are strictly monotone in the direction of this line. In particular, they take their maximum and minimum precisely at two antipodal points on the boundary of BB. We also prove that, for pp close to 22, minimizers are antisymmetric with respect to the hyperplane through the origin perpendicular to the symmetry axis, and that, once the symmetry axis is fixed, they are unique (up to multiplication by a constant). In space dimension two, we prove that minimizers are not antisymmetric for large pp

    Positive solutions to logistic type equations with harvesting

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    We use comparison principles, variational arguments and a truncation method to obtain positive solutions to logistic type equations with harvesting both in RN\mathbb{R}^N and in a bounded domain ΩRN\Omega\subset\mathbb{R}^N, with N3N\geq 3, when the carrying capacity of the environment is not constant. By relaxing the growth assumption on the coefficients of the differential equation we derive a new equation which is easily solved. The solution of this new equation is then used to produce a positive solution of our original problem

    Sign changing solutions for elliptic equations with critical growth in cylinder type domains

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    We prove the existence of positive and of nodal solutions for Δu=up2u+μuq2u-\Delta u = |u|^{p-2}u+\mu |u|^{q-2}u, uH01(Ω)u\in {\rm H_0^1}(\Omega), where μ>0\mu >0 and 2<q<p=2N(N2)2<q<p=2N(N-2), for a class of open subsets Ω\Omega of RN\mathbb{R}^N lying between two infinite cylinders.Comment: 13 page

    Convergence of a crystalline algorithm for the heat equation in one dimension and for the motion of a graph by weighted curvature

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    Motion by (weighted) mean curvature is a geometric evolution law for surfaces, representing steepest descent with respect to (an)isotropic surface energy. It has been proposed that this motion could be computed by solving the analogous evolution law using a "crystalline" approximation to the surface energy. We present the first convergence analysis for a numerical scheme of this type. Our treatment is restricted to one dimensional surfaces (curves in the plane) which are graphs. In this context, the scheme amounts to a new algorithm for solving quasilinear parabolic equations in one space dimension.Comment: 28 pages, 4 figure

    Existence and nonexistence of least energy solutions of the Neumann problem for a semilinear elliptic equation with critical Sobolev exponent and a critical lower-order perturbation

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    Let Ω\Omega be a smooth bounded domain in RN\mathbb{R}^{N}, with N5N\geq 5, a>0a>0, α0\alpha\geq 0 and 2=2NN22^*=\frac{2N}{N-2}. We show that the the exponent q=2(N1)N2q=\frac{2(N-1)}{N-2} plays a critical role regarding the existence of least energy (or ground state) solutions of the Neumann problem \left\{\begin{array}{ll} -\Delta u+au=u^{2^*-1}-\alpha u^{q-1}&\mbox{in}\ \Omega,\\ u>0&\mbox{in}\ \Omega,\\ \frac{\partial u}{\partial\nu}=0&\mbox{on}\ \partial\Omega. \end{array}\right. Namely, we prove that when q=2(N1)N2q=\frac{2(N-1)}{N-2} there exists an α0>0\alpha_{0}>0 such that the problem has a least energy solution if α<α0\alpha<\alpha_{0} and has no least energy solution if α>α0\alpha>\alpha_{0}.Comment: 30 page
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