Search results for "Operator"

showing 10 items of 1427 documents

Hermitian natural differential operators

1986

Hermitian symmetric spacePure mathematicsSpectral geometryHermitian manifoldSpectral theoremOperator theoryOperator normHermitian matrixFourier integral operatorMathematics
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Stability of radial symmetry for a Monge-Ampère overdetermined problem

2008

Recently the symmetry of solutions to overdetermined problems has been established for the class of Hessian operators, including the Monge-Ampère operator. In this paper we prove that the radial symmetry of the domain and of the solution to an overdetermined Dirichlet problem for the Monge-Ampère equation is stable under suitable perturbations of the data. © 2008 Fondazione Annali di Matematica Pura ed Applicata and Springer-Verlag.

Hessian matrixDirichlet problemoverdetermined problemMathematics::Complex VariablesApplied MathematicsMathematical analysisMathematics::Analysis of PDEsSymmetry in biologyMonge–Ampère equationMonge-Ampère equationComputer Science::Numerical AnalysisDomain (mathematical analysis)Symmetry (physics)Overdetermined systemsymbols.namesakeOperator (computer programming)Settore MAT/05 - Analisi MatematicasymbolsOverdetermined problemsStabilityIsoperimetric inequalityMathematics
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Comparison results for Hessian equations via symmetrization

2007

where the λ’s are the eigenvalues of the Hessian matrix D2u of u and Sk is the kth elementary symmetric function. For example, for k = 1, S1(Du) = 1u, while, for k = n, Sn(D 2u) = detD2u. Equations involving these operators, and some more general equations of the form F(λ1, . . . , λn) = f in , (1.2) have been widely studied by many authors, who restrict their considerations to convenient cones of solutions with respect to which the operator in (1.2) is elliptic. Following [25] we define the cone 0k of ellipticity for (1.1) to be the connected component containing the positive cone 0 = {λ ∈ R : λi > 0 ∀i = 1, . . . , n} of the set where Sk is positive. Thus 0k is an open, convex, symmetric…

Hessian matrixHessian equationsymmetrizationHessian operatorApplied MathematicsGeneral Mathematicscomparison resultHessian equationCombinatoricssymbols.namesakeOperator (computer programming)Cone (topology)Settore MAT/05 - Analisi MatematicaVertex (curve)symbolsSymmetrizationElementary symmetric polynomialMoser type inequalitiesAlgorithmEigenvalues and eigenvectorsMathematics
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Simplifying differential equations for multi-scale Feynman integrals beyond multiple polylogarithms

2017

In this paper we exploit factorisation properties of Picard-Fuchs operators to decouple differential equations for multi-scale Feynman integrals. The algorithm reduces the differential equations to blocks of the size of the order of the irreducible factors of the Picard-Fuchs operator. As a side product, our method can be used to easily convert the differential equations for Feynman integrals which evaluate to multiple polylogarithms to $\varepsilon$-form.

High Energy Physics - Theory010308 nuclear & particles physicsDifferential equationNumerical analysisGeneral Physics and AstronomyOrder (ring theory)FOS: Physical sciencesDecoupling (cosmology)Picard–Fuchs equation01 natural sciencesHigh Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)FactorizationHigh Energy Physics - Theory (hep-th)0103 physical sciencesComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONApplied mathematics010306 general physicsMathematicsNumerical partial differential equations
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The dyon charge in noncommutative gauge theories

2007

We present an explicit classical dyon solution for the noncommutative version of the Yang-Mills-Higgs model (in the Prasad-Sommerfield limit) with a tehta term. We show that the relation between classical electric and magnetic charges also holds in noncommutative space. Extending the Noether approach to the case of a noncommutative gauge theory, we analyze the effect of CP violation at the quantum level, induced both by the theta term and by noncommutativity and we prove that the Witten effect formula for the dyon charge remains the same as in ordinary space.

High Energy Physics - TheoryComputer Science::Machine LearningCiencias FísicasGeneral Physics and AstronomyFOS: Physical sciencesSpace (mathematics)Computer Science::Digital LibrariesStatistics::Machine Learningsymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheoryMathematics::Quantum AlgebraGauge theoryLimit (mathematics)Ciencias ExactasMathematical physicsPhysicsnoncommutative gauge theoryMathematics::Operator AlgebrasHigh Energy Physics::PhenomenologyFísicaCharge (physics)Noncommutative geometryDyonHigh Energy Physics - Theory (hep-th)Computer Science::Mathematical SoftwaresymbolsCP violationNoether's theorem
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Operator product expansion coefficients in the exact renormalization group formalism

2020

We study how to compute the operator product expansion coefficients in the exact renormalization group formalism. After discussing possible strategies, we consider some examples explicitly, within the $\epsilon$-expansions, for the Wilson-Fisher fixed points of the real scalar theory in $d=4-\epsilon$ dimensions and the Lee-Yang model in $d=6-\epsilon$ dimensions. Finally we discuss how our formalism may be extended beyond perturbation theory.

High Energy Physics - TheoryPhysics010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Scalar (mathematics)FOS: Physical sciencesFixed pointRenormalization group16. Peace & justiceComputer Science::Digital Libraries01 natural sciencesoperator product expansionfield theory in curved spaceFormalism (philosophy of mathematics)Formal aspects of field theoryHigh Energy Physics - Theory (hep-th)fixed point0103 physical sciencesLee-Yang modelOperator product expansionrenormalization group010306 general physicsMathematical physicsperturbation theory
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Composite operators in asymptotic safety

2017

We study the role of composite operators in the Asymptotic Safety program for quantum gravity. By including in the effective average action an explicit dependence on new sources we are able to keep track of operators which do not belong to the exact theory space and/or are normally discarded in a truncation. Typical examples are geometric operators such as volumes, lengths, or geodesic distances. We show that this set-up allows to investigate the scaling properties of various interesting operators via a suitable exact renormalization group equation. We test our framework in several settings, including Quantum Einstein Gravity, the conformally reduced Einstein-Hilbert truncation, and two dim…

High Energy Physics - TheoryPhysicsGeodesic010308 nuclear & particles physicsTruncationAsymptotic safety in quantum gravityFOS: Physical sciencesObservableGeneral Relativity and Quantum Cosmology (gr-qc)Operator theoryRenormalization group01 natural sciencesGeneral Relativity and Quantum CosmologyAction (physics)Theoretical physicsHigh Energy Physics - Theory (hep-th)Quantum mechanics0103 physical sciencesQuantum gravity010306 general physicsPhysical Review D
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Hopf algebras, renormalization and noncommutative geometry

1998

We explore the relation between the Hopf algebra associated to the renormalization of QFT and the Hopf algebra associated to the NCG computations of transverse index theory for foliations.

High Energy Physics - TheoryPhysicsMathematics::Rings and AlgebrasMathematics - Operator AlgebrasFOS: Physical sciencesStatistical and Nonlinear PhysicsHopf algebraNoncommutative geometryRenormalizationHigh Energy Physics - Theory (hep-th)Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Operator Algebras (math.OA)Mathematical PhysicsMathematical physics
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Superconformal mechanics, black holes, and non-linear realizations

1998

The OSp(2|2)-invariant planar dynamics of a D=4 superparticle near the horizon of a large mass extreme black hole is described by an N=2 superconformal mechanics, with the SO(2) charge being the superparticle's angular momentum. The {\it non-manifest} superconformal invariance of the superpotential term is shown to lead to a shift in the SO(2) charge by the value of its coefficient, which we identify as the orbital angular momentum. The full SU(1,1|2)-invariant dynamics is found from an extension to N=4 superconformal mechanics.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsAngular momentumSuperpotentialFOS: Physical sciencesMechanicsGeneral Relativity and Quantum Cosmology (gr-qc)Mathematical Physics (math-ph)General Relativity and Quantum CosmologyBlack holeHigh Energy Physics::TheoryRotating black holeHigh Energy Physics - Theory (hep-th)Total angular momentum quantum numberExtremal black holeAngular momentum couplingAngular momentum operatorMathematical Physics
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Supersymmetry in non commutative superspaces

2003

Non commutative superspaces can be introduced as the Moyal-Weyl quantization of a Poisson bracket for classical superfields. Different deformations are studied corresponding to constant background fields in string theory. Supersymmetric and non supersymmetric deformations can be defined, depending on the differential operators used to define the Poisson bracket. Some examples of deformed, 4 dimensional lagrangians are given. For extended superspace (N>1), some new deformations can be defined, with no analogue in the N=1 case.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsFOS: Physical sciencesFísicaSupersymmetrySuperspaceString theoryDifferential operatorNoncommutative geometryPoisson bracketQuantization (physics)High Energy Physics::TheoryNonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics - Theory (hep-th)Commutative propertyComputer Science::DatabasesParticle Physics - TheoryMathematical physics
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