Search results for "Variant"

showing 10 items of 1267 documents

Existence of common zeros for commuting vector fields on 3‐manifolds II. Solving global difficulties

2020

We address the following conjecture about the existence of common zeros for commuting vector fields in dimension three: if $X,Y$ are two $C^1$ commuting vector fields on a $3$-manifold $M$, and $U$ is a relatively compact open such that $X$ does not vanish on the boundary of $U$ and has a non vanishing Poincar\'e-Hopf index in $U$, then $X$ and $Y$ have a common zero inside $U$. We prove this conjecture when $X$ and $Y$ are of class $C^3$ and every periodic orbit of $Y$ along which $X$ and $Y$ are collinear is partially hyperbolic. We also prove the conjecture, still in the $C^3$ setting, assuming that the flow $Y$ leaves invariant a transverse plane field. These results shed new light on t…

Pure mathematicsConjectureGeneral Mathematics37C85010102 general mathematicsZero (complex analysis)Boundary (topology)Field (mathematics)Dynamical Systems (math.DS)01 natural sciences37C25Flow (mathematics)Relatively compact subspace0103 physical sciences58C30 (primary)FOS: MathematicsVector field010307 mathematical physics0101 mathematicsInvariant (mathematics)Mathematics - Dynamical Systems[MATH]Mathematics [math]57S05Mathematics
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Coprime actions and degrees of primitive inducers of invariant characters

2001

Let a finite group A act coprimely on a finite group G and χ ∈ Irr A(G). Isaacs, Lewis and Navarro proved that if G is nilpotent then the degrees of any two A-primitive characters of A-invariant subgroups of G inducing χ coincide. In this note we aim at extending this result by weakening the hypothesis on G.

Pure mathematicsCoprime integersGeneral MathematicsInvariant (mathematics)MathematicsBulletin of the Australian Mathematical Society
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Boundary quotients and ideals of Toeplitz C∗-algebras of Artin groups

2006

We study the quotients of the Toeplitz C*-algebra of a quasi-lattice ordered group (G,P), which we view as crossed products by a partial actions of G on closed invariant subsets of a totally disconnected compact Hausdorff space, the Nica spectrum of (G,P). Our original motivation and our main examples are drawn from right-angled Artin groups, but many of our results are valid for more general quasi-lattice ordered groups. We show that the Nica spectrum has a unique minimal closed invariant subset, which we call the boundary spectrum, and we define the boundary quotient to be the crossed product of the corresponding restricted partial action. The main technical tools used are the results of …

Pure mathematicsCovariant isometric representation01 natural sciencesToeplitz algebraCrossed productTotally disconnected space0103 physical sciencesFOS: MathematicsQuasi-lattice order0101 mathematicsInvariant (mathematics)Operator Algebras (math.OA)Artin groupQuotientMathematicsDiscrete mathematicsMathematics::Operator Algebras46L55010102 general mathematicsAmenable groupMathematics - Operator AlgebrasHausdorff spaceLength functionArtin group010307 mathematical physicsAnalysisJournal of Functional Analysis
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Biweights on Partial *-Algebras

2000

This chapter is devoted to the systematic investigation of biweights on partial *-algebras. These are a generalization of invariant positive sesquilinear forms that still allows a Gel’fand—Naĭmark—Segal (GNS) construction of representations. In Section 9.1, we apply this GNS construction for biweights and we obtain *-representations and cyclic vector representations of partial *-algebras, and we give some examples of biweights. Section 9.2 is devoted to the investigation of the Radon—Nikodým theorem and the Lebesgue decomposition theorem for biweights on partial *-algebras. In Section 9.3, we define regular and singular biweights on partial *-algebras and we characterize them with help of t…

Pure mathematicsDirect sumMathematics::Operator AlgebrasApplied MathematicsHilbert spacePartial *-algebrasLebesgue integrationLinear spansymbols.namesakeadmissible biweightsbiweightsSchwartz spaceBounded functionsymbolsGNS constructionInvariant (mathematics)weightsapproximately admissible biweightsAnalysisMathematicsDecomposition theoremJournal of Mathematical Analysis and Applications
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Dimension of self-affine sets for fixed translation vectors

2018

An affine iterated function system is a finite collection of affine invertible contractions and the invariant set associated to the mappings is called self-affine. In 1988, Falconer proved that, for given matrices, the Hausdorff dimension of the self-affine set is the affinity dimension for Lebesgue almost every translation vectors. Similar statement was proven by Jordan, Pollicott, and Simon in 2007 for the dimension of self-affine measures. In this article, we have an orthogonal approach. We introduce a class of self-affine systems in which, given translation vectors, we get the same results for Lebesgue almost all matrices. The proofs rely on Ledrappier-Young theory that was recently ver…

Pure mathematicsEuclidean spaceGeneral Mathematics010102 general mathematicsTranslation (geometry)Lebesgue integration01 natural sciencesMeasure (mathematics)010104 statistics & probabilitysymbols.namesakeIterated function systemHausdorff dimensionsymbolsAffine transformation0101 mathematicsInvariant (mathematics)MathematicsJournal of the London Mathematical Society
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Stability conditions and related filtrations for $(G,h)$-constellations

2017

Given an infinite reductive algebraic group $G$, we consider $G$-equivariant coherent sheaves with prescribed multiplicities, called $(G,h)$-constellations, for which two stability notions arise. The first one is analogous to the $\theta$-stability defined for quiver representations by King and for $G$-constellations by Craw and Ishii, but depending on infinitely many parameters. The second one comes from Geometric Invariant Theory in the construction of a moduli space for $(G,h)$-constellations, and depends on some finite subset $D$ of the isomorphy classes of irreducible representations of $G$. We show that these two stability notions do not coincide, answering negatively a question raise…

Pure mathematicsGeneral Mathematics01 natural sciencesHarder–Narasimhan filtrationCoherent sheafModuliMathematics - Algebraic GeometryMathematics::Algebraic Geometry0103 physical sciencesFOS: MathematicsComputer Science::General Literature14D20 14L24Representation Theory (math.RT)0101 mathematicsAlgebraic Geometry (math.AG)MathematicsComputer Science::Information Retrieval010102 general mathematicsQuiverAstrophysics::Instrumentation and Methods for AstrophysicsGIT quotientComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)16. Peace & justiceModuli spaceGIT quotientStability conditionAlgebraic groupIrreducible representationMSC: 14D20 14L24010307 mathematical physicsGeometric invariant theory[MATH.MATH-AG]Mathematics [math]/Algebraic Geometry [math.AG]Mathematics - Representation Theory
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Bounded elements in certain topological partial *-algebras

2011

We continue our study of topological partial *algebras, focusing our attention to the interplay between the various partial multiplications. The special case of partial *-algebras of operators is examined first, in particular the link between the strong and the weak multiplications, on one hand, and invariant positive sesquilinear (ips) forms, on the other. Then the analysis is extended to abstract topological partial *algebras, emphasizing the crucial role played by appropriate bounded elements, called $\M$-bounded. Finally, some remarks are made concerning representations in terms of the so-called partial GC*-algebras of operators.

Pure mathematicsGeneral MathematicsBounded elementMathematics - Rings and AlgebrasPrimary 47L60 Secondary 46H15Topologypartial *-algebrasAlgebraRings and Algebras (math.RA)Settore MAT/05 - Analisi MatematicaBounded functionFOS: Mathematicsbounded elementsSpecial caseInvariant (mathematics)Mathematics
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Quantization on the Virasoro group

1990

The quantization of the Virasoro group is carried out by means of a previously established group approach to quantization. We explicitly work out the two-cocycles on the Virasoro group as a preliminary step. In our scheme the carrier space for all the Virasoro representations is made out of polarized functions on the group manifold. It is proved that this space does not contain null vector states, even forc≦1, although it is not irreducible. The full reduction is achieved in a striaghtforward way by just taking a well defined invariant subspace ℋ(c, h), the orbit of the enveloping algebra through the vacuum, which is irreducible for any value ofc andh. ℋ(c, h) is a proper subspace of the sp…

Pure mathematicsGroup (mathematics)Quantization (signal processing)Invariant subspaceStatistical and Nonlinear Physics81S10ManifoldGroup representation17B68Algebra58F06Null vector81R10Algebra representation22E65Mathematical PhysicsSymplectic geometryMathematics
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Inner functions and local shape of orthonormal wavelets

2011

Abstract Conditions characterizing all orthonormal wavelets of L 2 ( R ) are given in terms of suitable orthonormal bases (ONBs) related with the translation and dilation operators. A particular choice of the ONBs, the so-called Haar bases, leads to new methods for constructing orthonormal wavelets from certain families of Hardy functions. Inner functions and the corresponding backward shift invariant subspaces articulate the structure of these families. The new algorithms focus on the local shape of the wavelet.

Pure mathematicsHardy spacesApplied MathematicsMathematical analysisWavelet transformHardy spaceLinear subspacesymbols.namesakeGeneralized Fourier seriesWaveletOrthonormal waveletssymbolsOrthonormal basisInvariant (mathematics)OrthonormalityInner functionsMathematicsApplied and Computational Harmonic Analysis
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An invariant analytic orthonormalization procedure with an application to coherent states

2007

We discuss a general strategy which produces an orthonormal set of vectors, stable under the action of a given set of unitary operators Aj, j=1,2,n, starting from a fixed normalized vector in H and from a set of unitary operators. We discuss several examples of this procedure and, in particular, we show how a set of coherentlike vectors can be produced and in which condition over the lattice spacing this can be done. © 2007 American Institute of Physics.

Pure mathematicsHilbert spaceFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)coherent statesUnitary stateMathematical OperatorsSet (abstract data type)symbols.namesakeUnit vectorsymbolsSet theoryInvariant (mathematics)Settore MAT/07 - Fisica MatematicaOrthonormalityComputer Science::DatabasesMathematical PhysicsMathematics
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