Search results for "35J60"

showing 10 items of 30 documents

Infinitely many solutions for p-Laplacian equation involving double critical terms and boundary geometry

2014

Let $1p^{2}+p,a(0)>0$ and $\Omega$ satisfies some geometry conditions if $0\in\partial\Omega$, say, all the principle curvatures of $\partial\Omega$ at $0$ are negative, then the above problem has infinitely many solutions.

Mathematics - Analysis of PDEsFOS: Mathematics35J60 35B33 35J60 35B33 35J60 35B33Analysis of PDEs (math.AP)
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Local Gauge Conditions for Ellipticity in Conformal Geometry

2013

In this article we introduce local gauge conditions under which many curvature tensors appearing in conformal geometry, such as the Weyl, Cotton, Bach, and Fefferman-Graham obstruction tensors, become elliptic operators. The gauge conditions amount to fixing an $n$-harmonic coordinate system and normalizing the determinant of the metric. We also give corresponding elliptic regularity results and characterizations of local conformal flatness in low regularity settings.

Mathematics - Differential Geometry53A30 (Primary) 53B20 35J60 (Secondary)General MathematicsCoordinate systemConformal mapCurvatureconformal geometry01 natural sciencessymbols.namesakeMathematics - Analysis of PDEs0103 physical sciencesFOS: Mathematics0101 mathematicsFlatness (mathematics)Mathematics010308 nuclear & particles physicsta111010102 general mathematicsMathematical analysisgauge conditionsGauge (firearms)Elliptic operatorDifferential Geometry (math.DG)symbolsWeyl transformationMathematics::Differential GeometryConformal geometryAnalysis of PDEs (math.AP)curvature tensors
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p-harmonic coordinates for H\"older metrics and applications

2015

We show that on any Riemannian manifold with H\"older continuous metric tensor, there exists a $p$-harmonic coordinate system near any point. When $p = n$ this leads to a useful gauge condition for regularity results in conformal geometry. As applications, we show that any conformal mapping between manifolds having $C^\alpha$ metric tensors is $C^{1+\alpha}$ regular, and that a manifold with $W^{1,n} \cap C^\alpha$ metric tensor and with vanishing Weyl tensor is locally conformally flat if $n \geq 4$. The results extend the works [LS14, LS15] from the case of $C^{1+\alpha}$ metrics to the H\"older continuous case. In an appendix, we also develop some regularity results for overdetermined el…

Mathematics - Differential Geometry53A30 (Primary) 35J60 35B65 (Secondary)
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Gradient regularity for elliptic equations in the Heisenberg group

2009

Abstract We give dimension-free regularity conditions for a class of possibly degenerate sub-elliptic equations in the Heisenberg group exhibiting super-quadratic growth in the horizontal gradient; this solves an issue raised in [J.J. Manfredi, G. Mingione, Regularity results for quasilinear elliptic equations in the Heisenberg group, Math. Ann. 339 (2007) 485–544], where only dimension dependent bounds for the growth exponent are given. We also obtain explicit a priori local regularity estimates, and cover the case of the horizontal p-Laplacean operator, extending some regularity proven in [A. Domokos, J.J. Manfredi, C 1 , α -regularity for p-harmonic functions in the Heisenberg group for …

Mathematics - Differential GeometryMathematics(all)Pure mathematicsp-LaplaceanGeneral MathematicsOperator (physics)Mathematical analysisDegenerate energy levelsHeisenberg groupWeak solutions35J60RegularityElliptic operatorMathematics - Analysis of PDEsDifferential Geometry (math.DG)Cover (topology)Euclidean geometryFOS: MathematicsHeisenberg groupExponentLinear equationAnalysis of PDEs (math.AP)MathematicsAdvances in Mathematics
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Existence and orbital stability of standing waves to nonlinear Schr��dinger system with partial confinement

2018

We are concerned with the existence of solutions to the following nonlinear Schr\"odinger system in $\mathbb{R}^3$: \begin{equation*} \left\{ \begin{aligned} -\Delta u_1 + (x_1^2+x_2^2)u_1&= \lambda_1 u_1 + \mu_1 |u_1|^{p_1 -2}u_1 + \beta r_1|u_1|^{r_1-2}u_1|u_2|^{r_2}, \\ -\Delta u_2 + (x_1^2+x_2^2)u_2&= \lambda_2 u_2 + \mu_2 |u_2|^{p_2 -2}u_2 +\beta r_2 |u_1|^{r_1}|u_2|^{r_2 -2}u_2, \end{aligned} \right. \end{equation*} under the constraint \begin{align*} \int_{\mathbb{R}^3}|u_1|^2 \, dx = a_1>0,\quad \int_{\mathbb{R}^3}|u_2|^2 \, dx = a_2>0, \end{align*} where $\mu_1, \mu_2, \beta >0, 2 1, r_1 + r_2 < \frac{10}{3}$. In the system, the parameters $\lambda_1, \lambda_2 \in \R$ are unknown …

PhysicsSequence010102 general mathematicsStatistical and Nonlinear Physics01 natural sciencesSchrödinger equation010101 applied mathematicsConstraint (information theory)symbols.namesakeNonlinear systemCompact spaceMathematics - Analysis of PDEsLagrange multiplier35J50 35J60symbolsFOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]0101 mathematicsComputingMilieux_MISCELLANEOUSMathematical PhysicsSchrödinger's catMathematical physicsEnergy functionalAnalysis of PDEs (math.AP)
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The behavior of solutions of a parametric weighted (p, q)-laplacian equation

2021

&lt;abstract&gt;&lt;p&gt;We study the behavior of solutions for the parametric equation&lt;/p&gt; &lt;p&gt;&lt;disp-formula&gt; &lt;label/&gt; &lt;tex-math id="FE1"&gt; \begin{document}$ -\Delta_{p}^{a_1} u(z)-\Delta_{q}^{a_2} u(z) = \lambda |u(z)|^{q-2} u(z)+f(z,u(z)) \quad \mbox{in } \Omega,\, \lambda &amp;gt;0, $\end{document} &lt;/tex-math&gt;&lt;/disp-formula&gt;&lt;/p&gt; &lt;p&gt;under Dirichlet condition, where $ \Omega \subseteq \mathbb{R}^N $ is a bounded domain with a $ C^2 $-boundary $ \partial \Omega $, $ a_1, a_2 \in L^\infty(\Omega) $ with $ a_1(z), a_2(z) &amp;gt; 0 $ for a.a. $ z \in \Omega $, $ p, q \in (1, \infty) $ and $ \Delta_{p}^{a_1}, \Delta_{q}^{a_2} $ are weighted …

Positive and negative solutionsGeneral MathematicsNodal solutionsLambdaOmegaCombinatoricssymbols.namesakeMathematics - Analysis of PDEsSettore MAT/05 - Analisi MatematicaQA1-939FOS: Mathematicspositive and negative solutionsResonant Carathéodory functionudc:517.956Physics35J20 35J60Spectrum (functional analysis)weighted (pWeighted (p q)-LaplacianDifferential operatorresonant Carathéodory functionweighted (pq)-LaplacianDirichlet boundary conditionBounded functionq)-laplacianDomain (ring theory)symbolsnodal solutionsParametric power termLaplace operatorMathematicsparametric power termAnalysis of PDEs (math.AP)
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Asymptotic Behaviors of Solutions to quasilinear elliptic Equations with critical Sobolev growth and Hardy potential

2015

Abstract Optimal estimates on the asymptotic behaviors of weak solutions both at the origin and at the infinity are obtained to the following quasilinear elliptic equations − Δ p u − μ | x | p | u | p − 2 u = Q ( x ) | u | N p N − p − 2 u , x ∈ R N , where 1 p N , 0 ≤ μ ( ( N − p ) / p ) p and Q ∈ L ∞ ( R N ) .

Pure mathematicsApplied Mathematicsmedia_common.quotation_subjectta111010102 general mathematicsMathematical analysisHardy's inequalitycomparison principleInfinity01 natural sciences010101 applied mathematicsSobolev spaceMathematics - Analysis of PDEs35J60 35B33FOS: Mathematicsquasilinear elliptic equationsasymptotic behaviors0101 mathematicsHardy's inequalityAnalysismedia_commonMathematicsAnalysis of PDEs (math.AP)
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Manifolds of quasiconformal mappings and the nonlinear Beltrami equation

2014

In this paper we show that the homeomorphic solutions to each nonlinear Beltrami equation $\partial_{\bar{z}} f = \mathcal{H}(z, \partial_{z} f)$ generate a two-dimensional manifold of quasiconformal mappings $\mathcal{F}_{\mathcal{H}} \subset W^{1,2}_{\mathrm{loc}}(\mathbb{C})$. Moreover, we show that under regularity assumptions on $\mathcal{H}$, the manifold $\mathcal{F}_{\mathcal{H}}$ defines the structure function $\mathcal{H}$ uniquely.

Pure mathematicsGeneral MathematicseducationMathematics::Analysis of PDEs01 natural sciencesBeltrami equationfunktioteoriaMathematics - Analysis of PDEsFOS: Mathematics0101 mathematicsComplex Variables (math.CV)30C62 (Primary) 35J60 35J46 (Secondary)MathematicsosittaisdifferentiaaliyhtälötPartial differential equationFunctional analysisMathematics - Complex Variables010102 general mathematicsStructure functionMathematics::Spectral Theory16. Peace & justiceManifold010101 applied mathematicsNonlinear systemmonistotAnalysisAnalysis of PDEs (math.AP)
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Nonlinear scalar field equations with general nonlinearity

2018

Consider the nonlinear scalar field equation \begin{equation} \label{a1} -\Delta{u}= f(u)\quad\text{in}~\mathbb{R}^N,\qquad u\in H^1(\mathbb{R}^N), \end{equation} where $N\geq3$ and $f$ satisfies the general Berestycki-Lions conditions. We are interested in the existence of positive ground states, of nonradial solutions and in the multiplicity of radial and nonradial solutions. Very recently Mederski [30] made a major advance in that direction through the development, in an abstract setting, of a new critical point theory for constrained functionals. In this paper we propose an alternative, more elementary approach, which permits to recover Mederski's results on the scalar field equation. T…

Pure mathematicsMathematics::Analysis of PDEsMonotonic function2010 MSC: 35J20 35J6001 natural sciencesMathematics - Analysis of PDEsFOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Mountain pass0101 mathematicsMathematicsgeographygeography.geographical_feature_category35J20 35J60Applied Mathematics010102 general mathematicsMultiplicity (mathematics)Monotonicity trickNonradial solutions010101 applied mathematicsNonlinear systemBerestycki-Lions nonlinearityBounded functionNonlinear scalar field equationsScalar fieldAnalysisAnalysis of PDEs (math.AP)
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Riesz and Wolff potentials and elliptic equations in variable exponent weak Lebesgue spaces

2015

Submitted by Alexandre Almeida (jaralmeida@ua.pt) on 2015-11-12T11:41:07Z No. of bitstreams: 1 RieszWolff_RIA.pdf: 159825 bytes, checksum: d99abdf3c874f47195619a31ff5c12c7 (MD5) Approved for entry into archive by Bella Nolasco(bellanolasco@ua.pt) on 2015-11-17T12:18:41Z (GMT) No. of bitstreams: 1 RieszWolff_RIA.pdf: 159825 bytes, checksum: d99abdf3c874f47195619a31ff5c12c7 (MD5) Made available in DSpace on 2015-11-17T12:18:41Z (GMT). No. of bitstreams: 1 RieszWolff_RIA.pdf: 159825 bytes, checksum: d99abdf3c874f47195619a31ff5c12c7 (MD5) Previous issue date: 2015-04

Pure mathematicsWolff potentialScale (ratio)Weak Lebesgue spaceVariable exponentMathematics::Classical Analysis and ODEsLebesgue's number lemmaNon-standard growth conditionIntegrability of solutionssymbols.namesakeMathematics - Analysis of PDEsReal interpolationFOS: MathematicsLp spaceMathematicsLaplace's equationMathematics::Functional AnalysisVariable exponentIntegrability estimatesRiesz potentialApplied MathematicsMathematical analysisFunctional Analysis (math.FA)Mathematics - Functional AnalysissymbolsRiesz potential47H99 (Primary) 46B70 46E30 35J60 31C45 (Secondary)Analysis of PDEs (math.AP)
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