Search results for "Diagram"

showing 10 items of 795 documents

Finite type invariants of knots in homology 3-spheres with respect to null LP-surgeries

2017

We study a theory of finite type invariants for null-homologous knots in rational homology 3-spheres with respect to null Lagrangian-preserving surgeries. It is an analogue in the setting of the rational homology of the Goussarov-Rozansky theory for knots in integral homology 3-spheres. We give a partial combinatorial description of the graded space associated with our theory and determine some cases when this description is complete. For null-homologous knots in rational homology 3-spheres with a trivial Alexander polynomial, we show that the Kricker lift of the Kontsevich integral and the Lescop equivariant invariant built from integrals in configuration spaces are universal finite type i…

Pure mathematicsAlexander polynomialPrimary: 57M27Homology (mathematics)01 natural sciencesHomology sphereMathematics::Algebraic TopologyMathematics - Geometric TopologyKnot (unit)Mathematics::K-Theory and Homologybeaded Jacobi diagramknot[MATH.MATH-GT]Mathematics [math]/Geometric Topology [math.GT]0103 physical sciencesFOS: Mathematics0101 mathematicsInvariant (mathematics)Mathematics::Symplectic Geometry3-manifoldhomology sphereMathematicsBorromean surgerycalculus010102 general mathematicsGeometric Topology (math.GT)Kontsevich integral16. Peace & justiceMathematics::Geometric TopologymanifoldsFinite type invariantnull-move57M27Finite type invariantLagrangian-preserving surgeryEquivariant map010307 mathematical physicsGeometry and Topology3-manifold
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A fuzzification of the category of M-valued L-topological spaces

2004

[EN] A fuzzy category is a certain superstructure over an ordinary category in which ”potential” objects and ”potential” morphisms could be such to a certain degree. The aim of this paper is to introduce a fuzzy category FTOP(L,M) extending the category TOP(L,M) of M-valued L- topological spaces which in its turn is an extension of the category TOP(L) of L-fuzzy topological spaces in Kubiak-Sostak’s sense. Basic properties of the fuzzy category FTOP(L,M) and its objects are studied.

Pure mathematicsFunctorHomotopy categoryDiagram (category theory)Mathematics::General Mathematicslcsh:Mathematicslcsh:QA299.6-433lcsh:Analysislcsh:QA1-939GL-monoid(LM)-fuzzy topologyPower-set operators(LM)-interior operatorMathematics::Category TheoryCategory of topological spacesBiproductUniversal propertyGeometry and TopologyM-valued L-topologyCategory of setsL-fuzzy category(LM)-neighborhood systemMathematicsInitial and terminal objectsApplied General Topology
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The cyclicity of the elliptic segment loops of the reversible quadratic Hamiltonian systems under quadratic perturbations

2004

Abstract Denote by Q H and Q R the Hamiltonian class and reversible class of quadratic integrable systems. There are several topological types for systems belong to Q H ∩ Q R . One of them is the case that the corresponding system has two heteroclinic loops, sharing one saddle-connection, which is a line segment, and the other part of the loops is an ellipse. In this paper we prove that the maximal number of limit cycles, which bifurcate from the loops with respect to quadratic perturbations in a conic neighborhood of the direction transversal to reversible systems (called in reversible direction), is two. We also give the corresponding bifurcation diagram.

Pure mathematicsIntegrable systemApplied MathematicsMathematical analysisBifurcation diagramEllipseHamiltonian systemsymbols.namesakeLine segmentQuadratic equationConic sectionCyclicity of elliptic segment loopssymbolsReversible quadratic Hamiltonian systemsHamiltonian (quantum mechanics)AnalysisMathematicsJournal of Differential Equations
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Hasse diagrams and orbit class spaces

2011

Abstract Let X be a topological space and G be a group of homeomorphisms of X. Let G ˜ be an equivalence relation on X defined by x G ˜ y if the closure of the G-orbit of x is equal to the closure of the G-orbit of y. The quotient space X / G ˜ is called the orbit class space and is endowed with the natural order inherited from the inclusion order of the closure of the classes, so that, if such a space is finite, one can associate with it a Hasse diagram. We show that the converse is also true: any finite Hasse diagram can be realized as the Hasse diagram of an orbit class space built from a dynamical system ( X , G ) where X is a compact space and G is a finitely generated group of homeomo…

Pure mathematicsMathematical analysisOrbit classClosure (topology)Hasse diagramTopological spaceGroup of homeomorphismsQuotient space (linear algebra)Hasse principleRealizationHomogeneous spaceCovering relationFinitely generated groupGeometry and TopologyHasse diagramMathematicsTopology and its Applications
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Nori’s Diagram Category

2017

We explain Nori’s construction of an abelian category attached to the representation of a diagram and establish some properties for it. The construction is completely formal. It mimics the standard construction of the Tannakian dual of a rigid tensor category with a fibre functor . Only, we do not have a tensor product or even a category but only what we should think of as the fibre functor.

Pure mathematicsMathematics::Algebraic GeometryFunctorTensor productMathematics::K-Theory and HomologyMathematics::Category TheoryTensor (intrinsic definition)DiagramAbelian categoryRepresentation (mathematics)Dual (category theory)Mathematics
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Representations of Affine Kac-Moody Algebras

1989

In the first chapter we explained how simple finite-dimensional Lie algebras can be completely characterized in terms of their Cartan matrices or Dynkin diagrams. The same holds for an arbitrary semisim-ple finite-dimensional Lie algebra. A semisimple Lie algebra is a direct sum of simple ideals which are pairwise orthogonal with respect to the Killing form. It follows that the Cartan matrix of a semisimple Lie algebra decomposes to a block diagonal form, each block representing a simple ideal. Similarly, the Dynkin diagram is a disconnected union of Dynkin diagrams of simple Lie algebras. Next we shall study certain infinite-dimensional Lie algebras which have many similarities with the si…

Pure mathematicsQuantum affine algebraDynkin diagramMathematics::Quantum AlgebraLie algebraCartan matrixNest algebraKilling formMathematics::Representation TheorySemisimple Lie algebraAffine Lie algebraMathematics
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Feynman-Kac formulae

2015

In this chapter, we establish the connection between the deterministic EIT forward problem and the class of reflecting diffusion processes. We proceed along the lines of the recent paper [137] by Piiroinen and the author: We derive Feynman-Kac formulae in terms of these processes for the solutions to the forward problems corresponding to the continuum model and the complete electrode model, respectively. These results extend the classical Feynman-Kac formulae for elliptic boundary value problems in smooth domains and with smooth coefficients which were obtained in the 1980s and 1990s using the Feller semigroup approach and Ito stochastic calculus. In contrast to this well-studied situation,…

Pure mathematicssymbols.namesakeClass (set theory)Continuum (measurement)Dirichlet formSemigroupsymbolsStochastic calculusFeynman diagramBoundary value problemMathematicsConnection (mathematics)
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Combining super-orthogonal space-frequency trellis coding, constellation shaping by shell mapping, and OFDM for high data rate broadband mobile commu…

2014

In this paper, we seamlessly combine three transmission techniques to design an improved performance broadband mobile communication system with two transmit antennas. In so doing, we took inspiration from the V.34 data modem toolbox designed for public switched telephone network. We modified the constellation shaping by shell mapping algorithm to apply it only to the orthogonal frequency division multiplexing (OFDM) frame sent by the first antenna, in such a way that the peak-to-average power ratio (PAPR) is also reduced for the second antenna. We use a 24-point quadrature amplitude modulation (QAM) signal constellation on each subcarrier, while the reference system employs 16 QAM for the s…

QAMEngineeringTransmission (telecommunications)business.industryOrthogonal frequency-division multiplexingBit error rateElectronic engineeringConstellation diagramElectrical and Electronic EngineeringTrellis modulationbusinessQuadrature amplitude modulationSubcarrierTransactions on Emerging Telecommunications Technologies
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Fold interaction and wavelength selection in 3D models of multilayer detachment folding

2014

Abstract Many fold-and-thrust belts are dominated by folding and exhibit a fairly regular fold-spacing. Yet, in map-view, the aspect ratio of doubly-plunging anticlines varies considerably from very elongated, and sometimes slightly curved, cylindrical folds to nearly circular, dome-like structures. In addition, the fold spacing often varies significantly around an average value. So far, it remains unclear whether these features are consistent with a folding instability. Therefore, we here study the dynamics of multilayer detachment folding, process by which shortening can be accommodated in thin-skinned fold-and-thrust belts. We start by analysing the physics of this process by using both …

Quantitative Biology::BiomoleculesDominant wavelengthAnticline3d modelGeometryFold (geology)InstabilityCrystallographyWavelengthGeophysicsGrowth rateGeologyEarth-Surface ProcessesPhase diagramTectonophysics
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Monte Carlo simulation of a lattice model for ternary polymer mixtures

1988

Monte Carlo studies of symmetrical polymer mixturesAB, modelled by selfavoiding walks withNA=NB=N steps on a simple cubic lattice, are presented for arbitrary concentrations of vacanciesφv in the range fromφv=0.2 toφv=0.8 and chain lengthsN≤64. We obtained the phase diagrams and the equation of state for three choices of the ratio ∈ / ∈AB (∈ being the energy between monomers of the same kind, ∈AB being the energy between different monomers). Flory-Huggins theory provides only a qualitative understanding of these results. If the equation of state is “fitted” with an effective Flory-Huggins parameterχeff, the latter turns out to be strongly dependent on both concentration and temperature.

Quantitative Biology::BiomoleculesEquation of statePolymers and PlasticsChemistryMonte Carlo methodThermodynamicsFlory–Huggins solution theoryCondensed Matter::Soft Condensed MatterColloid and Surface ChemistryMaterials ChemistryStatistical physicsPhysical and Theoretical ChemistryStructure factorTernary operationSelf-avoiding walkLattice model (physics)Phase diagramColloid & Polymer Science
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