Search results for "Differential operator"

showing 10 items of 70 documents

Higher-Order Differential Operators on a Lie Group and Quantization

1995

This talk is devoted mainly to the concept of higher-order polarization on a group, which is introduced in the framework of a Group Approach to Quantization, as a powerful tool to guarantee the irreducibility of quantizations and/or representations of Lie groups in those anomalous cases where the Kostant-Kirilov co-adjoint method or the Borel-Weyl-Bott representation algorithm do not succeed.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsGroup (mathematics)Quantization (signal processing)FOS: Physical sciencesLie groupAstronomy and AstrophysicsDifferential operatorAtomic and Molecular Physics and OpticsAlgebraHigh Energy Physics - Theory (hep-th)IrreducibilityOrder (group theory)Representation (mathematics)Mathematics::Representation Theory
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Solution of self-consistent equations for the N3LO nuclear energy density functional in spherical symmetry. The program hosphe (v1.02)

2010

Abstract We present solution of self-consistent equations for the N 3 LO nuclear energy density functional. We derive general expressions for the mean fields expressed as differential operators depending on densities and for the densities expressed in terms of derivatives of wave functions. These expressions are then specified to the case of spherical symmetry. We also present the computer program hosphe (v1.02), which solves the self-consistent equations by using the expansion of single-particle wave functions on the spherical harmonic oscillator basis. Program summary Program title: HOSPHE (v1.02) Catalogue identifier: AEGK_v1_0 Program summary URL: http://cpc.cs.qub.ac.uk/summaries/AEGK_…

PhysicsMathematical analysisGeneral Physics and AstronomySpherical harmonicsCPU timeDifferential operatorsymbols.namesakeHardware and ArchitectureQuantum electrodynamicsSelf-consistent mean fieldsymbolsNeutronCircular symmetryWave functionHamiltonian (quantum mechanics)Computer Physics Communications
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Improved constrained scheme for the Einstein equations: An approach to the uniqueness issue

2008

Uniqueness problems in the elliptic sector of constrained formulations of Einstein equations have a dramatic effect on the physical validity of some numerical solutions, for instance when calculating the spacetime of very compact stars or nascent black holes. The fully constrained formulation (FCF) proposed by Bonazzola, Gourgoulhon, Grandcl\'ement, and Novak is one of these formulations. It contains, as a particular case, the approximation of the conformal flatness condition (CFC) which, in the last ten years, has been used in many astrophysical applications. The elliptic part of the FCF basically shares the same differential operators as the elliptic equations in CFC scheme. We present he…

PhysicsNuclear and High Energy PhysicsGeneral relativityEquations of motionFOS: Physical sciencesConformal mapGeneral Relativity and Quantum Cosmology (gr-qc)Differential operatorGeneral Relativity and Quantum Cosmologysymbols.namesakeClassical mechanicsEinstein field equationssymbolsApplied mathematicsUniquenessEinsteinFlatness (mathematics)
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Weyl Asymptotics for the Damped Wave Equation

2019

The damped wave equation is closely related to non-self-adjoint perturbations of a self-adjoint operator P of the form $$\displaystyle P_\epsilon =P+i\epsilon Q. $$ Here, P is a semi-classical pseudodifferential operator of order 0 on L2(X), where we consider two cases: X = Rn and P has the symbol P ∼ p(x, ξ) + hp1(x, ξ) + ⋯ . in S(m), as in Sect. 6.1, where the description is valid also in the case n > 1. We assume for simplicity that the order function m(x, ξ) tends to + ∞, when (x, ξ) tends to ∞. We also assume that P is formally self-adjoint. Then by elliptic theory (and the ellipticity assumption on P) we know that P is essentially self-adjoint with purely discrete spectrum. X is a com…

PhysicsVolume formCombinatoricsOperator (physics)Order (ring theory)Function (mathematics)Differential operatorDiscrete spectrum
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Starlikeness Condition for a New Differential-Integral Operator

2020

A new differential-integral operator of the form I n f ( z ) = ( 1 &minus

Physicsconvex functionbest dominantPure mathematicsGeneral MathematicsOperator (physics)lcsh:Mathematicsstarlike functionDifferential operatorlcsh:QA1-939univalent functionanalytic functionComputer Science (miscellaneous)Convex functiondominantEngineering (miscellaneous)differential subordinationDifferential (mathematics)Analytic functionUnivalent functionMathematics
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Three solutions for parametric problems with nonhomogeneous (a,2)-type differential operators and reaction terms sublinear at zero

2019

Abstract We consider parametric Dirichlet problems driven by the sum of a Laplacian and a nonhomogeneous differential operator ( ( a , 2 ) -type equation) and with a reaction term which exhibits arbitrary polynomial growth and a nonlinear dependence on the parameter. We prove the existence of three distinct nontrivial smooth solutions for small values of the parameter, providing sign information for them: one is positive, one is negative and the third one is nodal.

PolynomialSublinear functionApplied Mathematics010102 general mathematicsMathematical analysisDifferential operator01 natural sciencesDirichlet distribution010101 applied mathematicssymbols.namesakeNonlinear systemSettore MAT/05 - Analisi Matematica(a2)-operator Constant sign solutions Nodal solutions Multiplicity of solutions Nonhomogeneous operatorsymbols0101 mathematicsLaplace operatorAnalysisSign (mathematics)MathematicsParametric statisticsJournal of Mathematical Analysis and Applications
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The behavior of solutions of a parametric weighted (p, q)-laplacian equation

2021

<abstract><p>We study the behavior of solutions for the parametric equation</p> <p><disp-formula> <label/> <tex-math id="FE1"> \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 >0, $\end{document} </tex-math></disp-formula></p> <p>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) > 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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Relative cohomology spaces for some osp($n|2$)-modules

2018

International audience; In this work, we describe the H-invariant, so(n)-relative cohomology of a natural class of osp(n|2)-modules M, for n ≠ 2. The Lie superalgebra osp(n|2) can be realized as a superalgebra of vector fields on the superline R1|n. This yields canonical actions on spaces of densities and differential operators on the superline. The above result gives the zero, first, and second cohomology spaces for these modules of densities and differential operators.

Pure mathematics010102 general mathematics[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]Zero (complex analysis)Statistical and Nonlinear PhysicsLie superalgebraDifferential operator01 natural sciencesCohomologySuperalgebraMathematics::Quantum Algebra0103 physical sciencesVector field010307 mathematical physics0101 mathematicsMathematics::Representation TheoryNatural classMathematical PhysicsMathematics
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Parameter dependence for the positive solutions of nonlinear, nonhomogeneous Robin problems

2020

We consider a parametric nonlinear Robin problem driven by a nonlinear nonhomogeneous differential operator plus an indefinite potential. The reaction term is $$(p-1)$$-superlinear but need not satisfy the usual Ambrosetti–Rabinowitz condition. We look for positive solutions and prove a bifurcation-type result for the set of positive solutions as the parameter $$\lambda >0$$ varies. Also we prove the existence of a minimal positive solution $$u_\lambda ^*$$ and determine the monotonicity and continuity properties of the map $$\lambda \rightarrow u_\lambda ^*$$.

Pure mathematicsAlgebra and Number TheoryApplied MathematicsMathematics::Analysis of PDEsMonotonic functionNonlinearDifferential operatorLambdaBifurcation-type resultTerm (time)Positive solutionSet (abstract data type)Computational MathematicsNonlinear systemSettore MAT/05 - Analisi MatematicaIndefinite potentialNonhomogeneous differential operatorGeometry and TopologySuperlinear reaction termAnalysisNonlinear regularity theoryParametric statisticsMathematicsRevista de la Real Academia de Ciencias Exactas, Físicas y Naturales. Serie A. Matemáticas
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Multiple Solutions with Sign Information for a Class of Coercive (p, 2)-Equations

2019

We consider a nonlinear Dirichlet equation driven by the sum of a p-Laplacian and of a Laplacian (a (p, 2)-equation). The hypotheses on the reaction f(z, x) are minimal and make the energy (Euler) functional of the problem coercive. We prove two multiplicity theorems producing three and four nontrivial smooth solutions, respectively, all with sign information. We apply our multiplicity results to the particular case of a class of parametric (p, 2)-equations.

Pure mathematicsClass (set theory)Constant sign solutionGeneral MathematicsNodal solutions010102 general mathematicsMultiplicity (mathematics)01 natural sciencesDirichlet distribution010101 applied mathematicssymbols.namesakeNonlinear systemSettore MAT/05 - Analisi MatematicaEuler's formulasymbolsHomotopy0101 mathematicsLaplace operator(p 2)-differential operatorCritical groupSign (mathematics)Parametric statisticsMathematicsBulletin of the Malaysian Mathematical Sciences Society
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