Search results for "Manifold"

showing 10 items of 415 documents

Reduction to finite dimensions of continuous systems having only a few amplified modes

2008

In the approach of Guckenheimer and Knobloch the amplitudes of trajectories on the unstable manifold 0 are the pivotal quantities. This places a certain restriction on the applicability of this approach, as only neighbourhoods of 0 of the unstable manifold of 0 are accessible, which have a one-to-one projection into their tangent at 0, the linear space spanned by the amplified modes. This restriction may be lifted, using the arc lengths of trajectories instead.

PhysicsAmplitudeTrivial solutionlawLinear spaceMathematical analysisTangentGeometryReduction (mathematics)Arc lengthManifold (fluid mechanics)Projection (linear algebra)law.invention
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Three physical quantum manifolds from the conformal group

1987

PhysicsConformal field theoryConformal symmetryQuantum electrodynamicsRicci-flat manifoldMass–energy equivalenceQuantumConformal geometryConformal groupMathematical physics
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Critical Attractor and Universality in a Renormalization Scheme for Three Frequency Hamiltonian Systems

1998

We study an approximate renormalization-group transformation to analyze the breakup of invariant tori for three degrees of freedom Hamiltonian systems. The scheme is implemented for the spiral mean torus. We find numerically that the critical surface is the stable manifold of a critical nonperiodic attractor. We compute scaling exponents associated with this fixed set, and find that they can be expected to be universal.

PhysicsCritical phenomenaGeneral Physics and AstronomyFOS: Physical sciencesTorusNonlinear Sciences - Chaotic DynamicsStable manifoldUniversality (dynamical systems)Hamiltonian systemRenormalizationAttractorChaotic Dynamics (nlin.CD)Critical exponentMathematics::Symplectic GeometryMathematical physics
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Presymplectic manifolds and conservation laws

2008

In this paper we make use of a new structure called seeded fibre bundle. This allows us to combine the symplectic formalism and general relativity. A theorem of existence is obtained and some examples and properties are studied.

PhysicsFormalism (philosophy of mathematics)Pure mathematicsConservation lawMathematics::Algebraic GeometryGeneral relativityFiber bundleHorizontal distributionMathematics::Symplectic GeometryMathematical physicsFibre typeSymplectic manifoldSymplectic geometry
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On the general structure of gauged Wess-Zumino-Witten terms

1998

The problem of gauging a closed form is considered. When the target manifold is a simple Lie group G, it is seen that there is no obstruction to the gauging of a subgroup H\subset G if we may construct from the form a cocycle for the relative Lie algebra cohomology (or for the equivariant cohomology), and an explicit general expression for these cocycles is given. The common geometrical structure of the gauged closed forms and the D'Hoker and Weinberg effective actions of WZW type, as well as the obstructions for their existence, is also exhibited and explained.

PhysicsHigh Energy Physics - TheoryMathematics - Differential GeometryNuclear and High Energy PhysicsPure mathematicsSimple Lie groupLie algebra cohomologyStructure (category theory)FOS: Physical sciencesMathematical Physics (math-ph)Type (model theory)Mathematics::Algebraic TopologyManifoldHigh Energy Physics::TheoryHigh Energy Physics - Theory (hep-th)Differential Geometry (math.DG)Mathematics::K-Theory and HomologyFOS: MathematicsEquivariant cohomologyGeneral expressionMathematical Physics
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Modular transformations of elliptic Feynman integrals

2021

We investigate the behaviour of elliptic Feynman integrals under modular transformations. This has a practical motivation: Through a suitable modular transformation we can achieve that the nome squared is a small quantity, leading to fast numerical evaluations. Contrary to the case of multiple polylogarithms, where it is sufficient to consider just variable transformations for the numerical evaluations of multiple polylogarithms, it is more natural in the elliptic case to consider a combination of a variable transformation (i.e. a modular transformation) together with a redefinition of the master integrals. Thus we combine a coordinate transformation on the base manifold with a basis transf…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsClass (set theory)Basis (linear algebra)010308 nuclear & particles physicsbusiness.industryCoordinate systemFOS: Physical sciencesModular designBase (topology)01 natural sciencesManifoldAlgebraHigh Energy Physics - PhenomenologyTransformation (function)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsbusinessVariable (mathematics)
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The Poisson Bracket Structure of the SL(2, R)/U(1) Gauged WZNW Model with Periodic Boundary Conditions

2000

The gauged SL(2, R)/U(1) Wess-Zumino-Novikov-Witten (WZNW) model is classically an integrable conformal field theory. A second-order differential equation of the Gelfand-Dikii type defines the Poisson bracket structure of the theory. For periodic boundary conditions zero modes imply non-local Poisson brackets which, nevertheless, can be represented by canonical free fields.

PhysicsHigh Energy Physics::TheoryPoisson bracketNonlinear Sciences::Exactly Solvable and Integrable SystemsIntegrable systemUniqueness theorem for Poisson's equationConformal field theoryDifferential equationPoisson manifoldGeneral Physics and AstronomyPeriodic boundary conditionsPoisson algebraMathematical physicsFortschritte der Physik
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Combinatorial Models in the Topological Classification of Singularities of Mappings

2018

The topological classification of finitely determined map germs \(f:(\mathbb R^n,0)\rightarrow (\mathbb R^p,0)\) is discrete (by a theorem due to R. Thom), hence we want to obtain combinatorial models which codify all the topological information of the map germ f. According to Fukuda’s work, the topology of such germs is determined by the link, which is obtained by taking the intersection of the image of f with a small enough sphere centered at the origin. If \(f^{-1}(0)=\{0\}\), then the link is a topologically stable map \(\gamma :S^{n-1}\rightarrow S^{p-1}\) (or stable if (n, p) are nice dimensions) and f is topologically equivalent to the cone of \(\gamma \). When \(f^{-1}(0)\ne \{0\}\)…

PhysicsImage (category theory)010102 general mathematicsDimension (graph theory)Boundary (topology)Stable map01 natural sciencesManifold010101 applied mathematicsCombinatoricsCone (topology)0101 mathematicsTopological conjugacyWord (group theory)
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APPROXIMATE INERTIAL MANIFOLDS FOR THERMODIFFUSION EQUATIONS

2004

In this paper, we consider the two dimensional equations of thermohydraulics, i.e. the coupled system of equations of fluid and temperature in the Boussinesq approximation. We construct a family of approximate Inertial Manifolds whose order decreases exponentially fast with respect to the dimension of the manifold. We give the explicit expression of the order of the constructed manifolds.

PhysicsInertial frame of referenceBenard problem inertial manifolds attractors dissipative systemsMathematical analysisSettore MAT/07 - Fisica MatematicaWaves and Stability in Continuous Media
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A Remark on an Overdetermined Problem in Riemannian Geometry

2016

Let (M, g) be a Riemannian manifold with a distinguished point O and assume that the geodesic distance d from O is an isoparametric function. Let \(\varOmega \subset M\) be a bounded domain, with \(O \in \varOmega \), and consider the problem \(\varDelta _p u = -1\ \mathrm{in}\ \varOmega \) with \(u=0\ \mathrm{on}\ \partial \varOmega \), where \(\varDelta _p\) is the p-Laplacian of g. We prove that if the normal derivative \(\partial _{\nu }u\) of u along the boundary of \(\varOmega \) is a function of d satisfying suitable conditions, then \(\varOmega \) must be a geodesic ball. In particular, our result applies to open balls of \(\mathbb {R}^n\) equipped with a rotationally symmetric metr…

PhysicsIsoparametric functionComparison principleGeodesic010102 general mathematicsRotationally symmetric spacesRiemannian manifoldRiemannian geometry01 natural sciencesRotationally symmetric spaceCombinatoricsOverdetermined systemsymbols.namesakeBounded function0103 physical sciencessymbolsComparison principle; Isoparametric functions; Overdetermined PDE; Riemannian Geometry; Rotationally symmetric spaces; Mathematics (all)Isoparametric functionsMathematics (all)Overdetermined PDEMathematics::Differential Geometry010307 mathematical physics0101 mathematicsRiemannian Geometry
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