Search results for "Symplectic geometry"

showing 9 items of 209 documents

Rotation Forms and Local Hamiltonian Monodromy

2017

International audience; The monodromy of torus bundles associated with completely integrable systems can be computed using geometric techniques (constructing homology cycles) or analytic arguments (computing discontinuities of abelian integrals). In this article, we give a general approach to the computation of monodromy that resembles the analytical one, reducing the problem to the computation of residues of polar 1-forms. We apply our technique to three celebrated examples of systems with monodromy (the champagne bottle, the spherical pendulum, the hydrogen atom) and to the case of non-degenerate focus-focus singularities, re-obtaining the classical results. An advantage of this approach …

[ MATH ] Mathematics [math]Pure mathematicsIntegrable systemFOCUS-FOCUS SINGULARITIESmath-phFOS: Physical sciencesDynamical Systems (math.DS)Homology (mathematics)01 natural sciencesSingularityMathematics::Algebraic Geometrymath.MPSYSTEMS0103 physical sciencesFOS: Mathematics0101 mathematicsAbelian groupMathematics - Dynamical Systems[MATH]Mathematics [math]010306 general physicsMathematics::Symplectic GeometryMathematical PhysicsMathematicsNEIGHBORHOODS[PHYS]Physics [physics][ PHYS ] Physics [physics]010102 general mathematicsSpherical pendulumStatistical and Nonlinear PhysicsTorusMathematical Physics (math-ph)37JxxMonodromyStatistical and Nonlinear Physics; Mathematical PhysicsGravitational singularityPOINTSmath.DS
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THE HOMOLOGY OF DIGRAPHS AS A GENERALIZATION OF HOCHSCHILD HOMOLOGY

2010

J. Przytycki has established a connection between the Hochschild homology of an algebra $A$ and the chromatic graph homology of a polygon graph with coefficients in $A$. In general the chromatic graph homology is not defined in the case where the coefficient ring is a non-commutative algebra. In this paper we define a new homology theory for directed graphs which takes coefficients in an arbitrary $A-A$ bimodule, for $A$ possibly non-commutative, which on polygons agrees with Hochschild homology through a range of dimensions.

[ MATH.MATH-GT ] Mathematics [math]/Geometric Topology [math.GT]57M15 16E40 05C20Homology (mathematics)[ MATH.MATH-CO ] Mathematics [math]/Combinatorics [math.CO]Mathematics::Algebraic Topology01 natural sciencesCombinatoricsMathematics - Geometric TopologyMathematics::K-Theory and Homology[MATH.MATH-GT]Mathematics [math]/Geometric Topology [math.GT][MATH.MATH-CO]Mathematics [math]/Combinatorics [math.CO][ MATH.MATH-KT ] Mathematics [math]/K-Theory and Homology [math.KT]0103 physical sciencesFOS: MathematicsMathematics - CombinatoricsChromatic scale0101 mathematicsMathematics::Symplectic GeometryMathematicsAlgebra and Number TheoryHochschild homologyApplied Mathematics010102 general mathematicsGeometric Topology (math.GT)K-Theory and Homology (math.KT)Directed graphMathematics::Geometric TopologyGraphMathematics - K-Theory and HomologyPolygon[MATH.MATH-KT]Mathematics [math]/K-Theory and Homology [math.KT]BimoduleCombinatorics (math.CO)010307 mathematical physicsJournal of Algebra and Its Applications
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3-manifolds which are orbit spaces of diffeomorphisms

2008

Abstract In a very general setting, we show that a 3-manifold obtained as the orbit space of the basin of a topological attractor is either S 2 × S 1 or irreducible. We then study in more detail the topology of a class of 3-manifolds which are also orbit spaces and arise as invariants of gradient-like diffeomorphisms (in dimension 3). Up to a finite number of exceptions, which we explicitly describe, all these manifolds are Haken and, by changing the diffeomorphism by a finite power, all the Seifert components of the Jaco–Shalen–Johannson decomposition of these manifolds are made into product circle bundles.

[ MATH.MATH-GT ] Mathematics [math]/Geometric Topology [math.GT]Seifert fibrationsClass (set theory)Pure mathematicsGradient-like diffeomorphism[ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS]Dimension (graph theory)[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS][MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Space (mathematics)01 natural sciences[MATH.MATH-GT]Mathematics [math]/Geometric Topology [math.GT]0103 physical sciencesAttractorJaco–Shalen–Johannson decomposition0101 mathematicsFinite setMathematics::Symplectic Geometry[MATH.MATH-GT] Mathematics [math]/Geometric Topology [math.GT]Mathematics010102 general mathematicsMathematical analysisMathematics::Geometric Topology3-manifoldsProduct (mathematics)010307 mathematical physicsGeometry and TopologyDiffeomorphismOrbit (control theory)
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Topological Hopf algebras, quantum groups and deformation quantization

2003

After a presentation of the context and a brief reminder of deformation quantization, we indicate how the introduction of natural topological vector space topologies on Hopf algebras associated with Poisson Lie groups, Lie bialgebras and their doubles explains their dualities and provides a comprehensive framework. Relations with deformation quantization and applications to the deformation quantization of symmetric spaces are described

[ MATH.MATH-QA ] Mathematics [math]/Quantum Algebra [math.QA]quantum groups[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]FOS: Physical sciences[ MATH.MATH-SG ] Mathematics [math]/Symplectic Geometry [math.SG]topological vector spacesMathematical Physics (math-ph)[MATH.MATH-SG]Mathematics [math]/Symplectic Geometry [math.SG]deformation quantizationMathematics - Symplectic GeometryHopf algebras54C40 14E20 (primary) 46E25 20C20 (secondary)[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: Mathematics[MATH.MATH-QA]Mathematics [math]/Quantum Algebra [math.QA]Quantum Algebra (math.QA)Symplectic Geometry (math.SG)Mathematical Physics
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A Symplectic Kovacic's Algorithm in Dimension 4

2018

Let $L$ be a $4$th order differential operator with coefficients in $\mathbb{K}(z)$, with $\mathbb{K}$ a computable algebraically closed field. The operator $L$ is called symplectic when up to rational gauge transformation, the fundamental matrix of solutions $X$ satisfies $X^t J X=J$ where $J$ is the standard symplectic matrix. It is called projectively symplectic when it is projectively equivalent to a symplectic operator. We design an algorithm to test if $L$ is projectively symplectic. Furthermore, based on Kovacic's algorithm, we design an algorithm that computes Liouvillian solutions of projectively symplectic operators of order $4$. Moreover, using Klein's Theorem, algebraic solution…

[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]010102 general mathematicsDynamical Systems (math.DS)Differential operator01 natural sciencesSymplectic matrixDifferential Galois theory34M15Operator (computer programming)Fundamental matrix (linear differential equation)Mathematics - Symplectic Geometry0103 physical sciencesFOS: MathematicsSymplectic Geometry (math.SG)010307 mathematical physicsMathematics - Dynamical Systems0101 mathematicsAlgebraically closed fieldAlgebraic numberMathematics::Symplectic GeometryAlgorithmMathematicsSymplectic geometryProceedings of the 2018 ACM International Symposium on Symbolic and Algebraic Computation
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Minimal number of periodic orbits for nonsingular Morse-Smale flows in odd dimension

2020

We compute the minimal number p_min of closed orbits of any Morse-Smale flow on any compact odd-dimensional manifold with boundary in terms of some given homological information. The underlying algorithm is based on optimization theory in network flows and transport systems. Such a number p_min is a lower bound in the general case but we provide, for any initial homological data, a Morse-Smale model for which p_min is attained. We also apply our techniques to the problem of the continuation of Lyapnov graphs to Lyapnov graphs of Smale type.

[MATH] Mathematics [math][MATH]Mathematics [math]Mathematics::Algebraic TopologyMathematics::Symplectic GeometryMathematics::Geometric Topology
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Algebraic models of the real affine plane

2017

We introduce a new invariant, the real (logarithmic)-Kodaira dimension, that allows to distinguish smooth real algebraic surfaces up to birational diffeomorphism. As an application, we construct infinite families of smooth rational real algebraic surfaces with trivial homology groups, whose real loci are diffeomorphic to $\mathbb{R}^2$, but which are pairwise not birationally diffeomorphic. There are thus infinitely many non-trivial models of the real affine plane, contrary to the compact case.

birational diffeomorphismaffine complexificationMathematics::Algebraic Geometry14R05 14R25 14E05 14P25 14J26.affine surface[MATH.MATH-AG] Mathematics [math]/Algebraic Geometry [math.AG]rational fibrationReal algebraic model[MATH.MATH-AG]Mathematics [math]/Algebraic Geometry [math.AG]Mathematics::Symplectic Geometry[ MATH.MATH-AG ] Mathematics [math]/Algebraic Geometry [math.AG]
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An unbounded family of log Calabi–Yau pairs

2016

We give an explicit example of log Calabi-Yau pairs that are log canonical and have a linearly decreasing Euler characteristic. This is constructed in terms of a degree two covering of a sequence of blow ups of three dimensional projective bundles over the Segre-Hirzebruch surfaces ${\mathbb F}_n$ for every positive integer $n$ big enough.

geography of threefoldSequenceDegree (graph theory)Projective bundleGeneral Mathematics14J30 14J32 14J60CombinatoricsMathematics - Algebraic Geometrysymbols.namesakeMathematics::Algebraic Geometryprojective bundlesIntegerEuler characteristicLog Calabi-Yau pairFOS: MathematicssymbolsCalabi–Yau manifoldSettore MAT/03 - GeometriaAlgebraic Geometry (math.AG)Mathematics::Symplectic GeometryMAT/03 - GEOMETRIAMathematicsRendiconti Lincei - Matematica e Applicazioni
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Comparison of frictional resistance between passive self-ligating brackets and slide-type low-friction ligature brackets during the alignment and lev…

2019

Background To compare the frictional resistance between passive self-ligating brackets and conventional brackets with low-friction ligature under bracket/archwire and root/bone interface during dental alignment and leveling. Material and methods A tridimensional model of the maxilla and teeth of a patient treated with conventional brackets, and slide ligatures was generated employing the SolidWorks modeling software. SmartClip self-ligating brackets and Logic Line conventional brackets were assembled with slide low-friction ligatures, utilizing archwires with different diameters and alloys used for the alignment and leveling stage. Friction caused during the bracket/archwire interface and s…

musculoskeletal diseasesModeling softwareMaterials sciencemedicine.medical_treatmentPhysics::Medical PhysicsOrthodonticsLow frictionStress (mechanics)03 medical and health sciences0302 clinical medicineMathematics::Quantum Algebramedicine030223 otorhinolaryngologyLigatureGeneral DentistryMathematics::Symplectic GeometryOrthodontic FrictionOrthodonticsOrthodontic wireintegumentary systemResearchBracket030206 dentistry:CIENCIAS MÉDICAS [UNESCO]musculoskeletal systemNonlinear Sciences::Exactly Solvable and Integrable SystemsUNESCO::CIENCIAS MÉDICASFrictional resistancehuman activitiesJournal of Clinical and Experimental Dentistry
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