Search results for "FOS: Mathematics"

showing 10 items of 1448 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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Spectral approach to D-bar problems

2017

We present the first numerical approach to D-bar problems having spectral convergence for real analytic, rapidly decreasing potentials. The proposed method starts from a formulation of the problem in terms of an integral equation that is numerically solved with Fourier techniques. The singular integrand is regularized analytically. The resulting integral equation is approximated via a discrete system that is solved with Krylov methods. As an example, the D-bar problem for the Davey-Stewartson II equations is considered. The result is used to test direct numerical solutions of the PDE.© 2017 Wiley Periodicals, Inc.

[ MATH ] Mathematics [math]Spectral approachInverse conductivity problemBar (music)General MathematicsElectrical-impedance tomographyFOS: Physical sciences2 dimensions010103 numerical & computational mathematics01 natural sciencesDiscrete systemsymbols.namesakeConvergence (routing)FOS: MathematicsApplied mathematicsUniquenessStewartson-ii equationsMathematics - Numerical Analysis0101 mathematics[MATH]Mathematics [math]Electrical impedance tomographyReconstruction algorithmsNumerical-solutionMathematicsNonlinear Sciences - Exactly Solvable and Integrable SystemsApplied MathematicsNumerical Analysis (math.NA)Integral equation010101 applied mathematicsFourier transformsymbolsUniquenessExactly Solvable and Integrable Systems (nlin.SI)
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Geometric représentations of the braid groups

2010

We show that the morphisms from the braid group with n strands in the mapping class group of a surface with a possible non empty boundary, assuming that its genus is smaller or equal to n/2 are either cyclic morphisms (their images are cyclic groups), or transvections of monodromy morphisms (up to multiplication by an element in the centralizer of the image, the image of a standard generator of the braid group is a Dehn twist, and the images of two consecutive standard generators are two Dehn twists along two curves intersecting in one point). As a corollary, we determine the endomorphisms, the injective endomorphisms, the automorphisms and the outer automorphism group of the following grou…

[ MATH ] Mathematics [math]rigidité[ MATH.MATH-GR ] Mathematics [math]/Group Theory [math.GR]morphisme de monodromieification de Nielsen Thurstonbraid groupGroup Theory (math.GR)[MATH] Mathematics [math]groupe de difféotopies[MATH.MATH-GR]Mathematics [math]/Group Theory [math.GR]monodromieFOS: Mathematicssurface[MATH]Mathematics [math]représentation géométriquetransvectionmonodromymapping class groupMathematics::Geometric TopologyrigidityNielsen-Thurstongroupe de tressesAMS Subject Classification: Primary 20F38 57M07. Secondary 57M99 20F36 20E36 57M05.mapping groupMathematics - Group Theorygroupe de diffétopies
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Unfolding of saddle-nodes and their Dulac time

2016

Altres ajuts: UNAB10-4E-378, co-funded by ERDF "A way to build Europe" and by the French ANR-11-BS01-0009 STAAVF. In this paper we study unfoldings of saddle-nodes and their Dulac time. By unfolding a saddle-node, saddles and nodes appear. In the first result (Theorem A) we give a uniform asymptotic expansion of the trajectories arriving at the node. Uniformity is with respect to all parameters including the unfolding parameter bringing the node to a saddle-node and a parameter belonging to a space of functions. In the second part, we apply this first result for proving a regularity result (Theorem B) on the Dulac time (time of Dulac map) of an unfolding of a saddle-node. This result is a b…

[ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS][MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]Block (permutation group theory)Dynamical Systems (math.DS)Space (mathematics)01 natural sciencesCombinatoricsQuadratic equationFOS: MathematicsMathematics - Dynamical Systems0101 mathematicsBifurcationSaddleMathematicsPeriod functionApplied MathematicsUnfolding of a saddle-node010102 general mathematics16. Peace & justice010101 applied mathematicsMSC: 34C07Asymptotic expansions34C07Node (circuits)Asymptotic expansionAnalysis
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A Franks' lemma that preserves invariant manifolds

2009

A well-known lemma by John Franks asserts that one obtains any perturbation of the derivative of a diffeomorphism along a periodic orbit by a $C^1$-perturbation of the whole diffeomorphism on a small neighbourhood of the orbit. However, one does not control where the invariant manifolds of the orbit are, after perturbation. We show that if the perturbated derivative is obtained by an isotopy along which some strong stable/unstable manifolds of some dimensions exist, then the Franks perturbation can be done preserving the corresponding stable/unstable semi-local manifolds. This is a general perturbative tool in $C^1$-dynamics that has many consequences. We give simple examples of such conseq…

[ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS][MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]FOS: Mathematics37C25 37C29 37C20 37D10[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Dynamical Systems (math.DS)Mathematics - Dynamical Systems
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A simple algorithm for finding short sigma-definite representatives

2010

We describe a new algorithm which for each braid returns a quasi-geodesic sigma-definite word representative, defined as a braid word in which the generator sigma_i with maximal index i appears either only positively or only negatively.

[ MATH.MATH-GR ] Mathematics [math]/Group Theory [math.GR]Braid groupbraid monoids20F3620M0506F05Group Theory (math.GR)02 engineering and technology01 natural sciences[MATH.MATH-GR]Mathematics [math]/Group Theory [math.GR]Mathematics::Group TheoryMathematics::Category TheoryMathematics::Quantum AlgebraFOS: MathematicsBraidBraid group0101 mathematicsSIMPLE algorithmMathematicsDiscrete mathematicsGenerator (computer programming)algorithmAlgebra and Number Theory010102 general mathematicsSigmaComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)021001 nanoscience & nanotechnologyMathematics::Geometric Topologybraid orderingIndex (publishing)0210 nano-technologyMathematics - Group TheoryWord (computer architecture)Journal of Algebra
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IRREDUCIBLE COXETER GROUPS

2004

We prove that a non-spherical irreducible Coxeter group is (directly) indecomposable and that an indefinite irreducible Coxeter group is strongly indecomposable in the sense that all its finite index subgroups are (directly) indecomposable. Let W be a Coxeter group. Write W = WX1 × ⋯ × WXb × WZ3, where WX1, … , WXb are non-spherical irreducible Coxeter groups and WZ3 is a finite one. By a classical result, known as the Krull–Remak–Schmidt theorem, the group WZ3 has a decomposition WZ3 = H1 × ⋯ × Hq as a direct product of indecomposable groups, which is unique up to a central automorphism and a permutation of the factors. Now, W = WX1 × ⋯ × WXb × H1 × ⋯ × Hq is a decomposition of W as a dir…

[ MATH.MATH-GR ] Mathematics [math]/Group Theory [math.GR]General MathematicsGroup Theory (math.GR)0102 computer and information sciencesPoint group01 natural sciences[MATH.MATH-GR]Mathematics [math]/Group Theory [math.GR]CombinatoricsMathematics::Group TheoryFOS: Mathematics0101 mathematicsLongest element of a Coxeter groupMathematics::Representation Theory[MATH.MATH-GR] Mathematics [math]/Group Theory [math.GR]MathematicsMathematics::CombinatoricsCoxeter notationMathematics::Rings and Algebras010102 general mathematicsCoxeter group010201 computation theory & mathematicsCoxeter complexArtin group20F55Indecomposable moduleMathematics - Group TheoryCoxeter elementInternational Journal of Algebra and Computation
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Ping-pong configurations and circular orders on free groups

2017

We discuss actions of free groups on the circle with "ping-pong" dynamics; these are dynamics determined by a finite amount of combinatorial data, analogous to Schottky domains or Markov partitions. Using this, we show that the free group $F_n$ admits an isolated circular order if and only if n is even, in stark contrast with the case for linear orders. This answers a question from (Mann, Rivas, 2016). Inspired by work of Alvarez, Barrientos, Filimonov, Kleptsyn, Malicet, Menino and Triestino, we also exhibit examples of "exotic" isolated points in the space of all circular orders on $F_2$. Analogous results are obtained for linear orders on the groups $F_n \times \mathbb{Z}$.

[ MATH.MATH-GR ] Mathematics [math]/Group Theory [math.GR][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS][MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]MSC2010: Primary 20F60 57M60. Secondary 20E05 37C85 37E05 37E10 57M60.Extension (predicate logic)Group Theory (math.GR)Dynamical Systems (math.DS)Space (mathematics)20F60 57M60[MATH.MATH-GR]Mathematics [math]/Group Theory [math.GR]CombinatoricsFree groupsOne-dimensional dynamicsFree groupPing pongFOS: MathematicsDiscrete Mathematics and CombinatoricsOrder (group theory)Geometry and TopologyMathematics - Dynamical SystemsMathematics - Group TheoryMathematicsOrders on groups
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Free vs. Locally Free Kleinian Groups

2015

Abstract We prove that Kleinian groups whose limit sets are Cantor sets of Hausdorff dimension < < 1 are free. On the other hand we construct for any ε > > 0 an example of a non-free purely hyperbolic Kleinian group whose limit set is a Cantor set of Hausdorff dimension < < 1 + + ε.

[ MATH.MATH-GT ] Mathematics [math]/Geometric Topology [math.GT]0209 industrial biotechnologyPure mathematicsMathematics::Dynamical SystemsGeneral MathematicsMathematics::General TopologyGroup Theory (math.GR)02 engineering and technology01 natural sciencesMathematics - Geometric Topology020901 industrial engineering & automationDimension (vector space)[MATH.MATH-GT]Mathematics [math]/Geometric Topology [math.GT]FOS: MathematicsLimit (mathematics)topologia0101 mathematicsMathematicsApplied Mathematics010102 general mathematicsryhmäteoriaGeometric Topology (math.GT)16. Peace & justiceMathematics::Geometric TopologyKleinian groupsCantor setTheoryofComputation_MATHEMATICALLOGICANDFORMALLANGUAGESHausdorff dimensionComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLimit setMathematics - Group Theory
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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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