Search results for " function"

showing 10 items of 9395 documents

Assouad dimension, Nagata dimension, and uniformly close metric tangents

2013

We study the Assouad dimension and the Nagata dimension of metric spaces. As a general result, we prove that the Nagata dimension of a metric space is always bounded from above by the Assouad dimension. Most of the paper is devoted to the study of when these metric dimensions of a metric space are locally given by the dimensions of its metric tangents. Having uniformly close tangents is not sufficient. What is needed in addition is either that the tangents have dimension with uniform constants independent from the point and the tangent, or that the tangents are unique. We will apply our results to equiregular subRiemannian manifolds and show that locally their Nagata dimension equals the to…

Pure mathematicssub-Riemannian manifoldsGeneral Mathematics54F45 (Primary) 53C23 54E35 53C17 (Secondary)01 natural sciencessymbols.namesakeMathematics - Geometric TopologyDimension (vector space)Mathematics - Metric Geometry0103 physical sciencesFOS: MathematicsMathematics (all)assouad dimensionMathematics::Metric GeometryPoint (geometry)0101 mathematicsMathematics010102 general mathematicsta111TangentMetric Geometry (math.MG)Geometric Topology (math.GT)16. Peace & justiceMetric dimensionAssouad dimension; Metric tangents; Nagata dimension; Sub-Riemannian manifolds; Mathematics (all)Metric spaceBounded functionNagata dimensionMetric (mathematics)symbols010307 mathematical physicsMathematics::Differential Geometrymetric tangentsLebesgue covering dimension
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Normed Quasi *-Algebras: Bounded Elements and Spectrum

2020

Bounded elements of a Banach quasi *-algebra are intended to be those, whose images under every *-representation are bounded operators in a Hilbert space. This rough idea can be developed in several ways, as we shall see in the present chapter. These notions lead us to discuss a convenient concept of spectrum of an element in this context.

Pure mathematicssymbols.namesakeBounded functionSpectrum (functional analysis)Hilbert spacesymbolsContext (language use)Element (category theory)Representation (mathematics)Mathematics
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Rate of Mixing for Equilibrium States in Negative Curvature and Trees

2021

In this survey based on the recent book by the three authors, we recall the Patterson-Sullivan construction of equilibrium states for the geodesic flow on negatively curved orbifolds or tree quotients, and discuss their mixing properties, emphasizing the rate of mixing for (not necessarily compact) tree quotients via coding by countable (not necessarily finite) topological shifts. We give a new construction of numerous nonuniform tree lattices such that the (discrete time) geodesic flow on the tree quotient is exponentially mixing with respect to the maximal entropy measure: we construct examples whose tree quotients have an arbitrary space of ends or an arbitrary (at most exponential) grow…

Pure mathematicssymbols.namesakeExponential growthDiscrete time and continuous timeThermodynamic equilibriumsymbolsCountable setNegative curvatureGibbs measureQuotientMathematicsExponential function
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Functions of One Variable

2019

A classical result of Fatou gives that every bounded holomorphic function on the disc has radial limits for almost every point in the torus, and the limit function belongs to the Hardy space H_\infty of the torus. This property is no longer true when we consider vector-valued functions. The Banach spaces X for which this property is satisfied are said to have the analytic Radon-Nikodym property (ARNP). Some important equivalent reformulations of ARNP are studied in this chapter. Among others, X has ARNP if and only if each X-valued H_p- function f on the disc has radial limits almost everywhere on the torus (and not only H_\infty-functions). Even more, in this case each such f has non-tange…

Pure mathematicssymbols.namesakeSubharmonic functionBounded functionBanach spaceHolomorphic functionsymbolsAlmost everywhereTorusHardy–Littlewood maximal functionHardy spaceMathematics
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Green’s function and existence of solutions for a third-order three-point boundary value problem

2019

The solutions of third-order three-point boundary value problem x‘‘‘ + f(t, x) = 0, t ∈ [a, b], x(a) = x‘(a) = 0, x(b) = kx(η), where η ∈ (a, b), k ∈ R, f ∈ C([a, b] × R, R) and f(t, 0) ≠ 0, are the subject of this investigation. In order to establish existence and uniqueness results for the solutions, attention is focused on applications of the corresponding Green’s function. As an application, also one example is given to illustrate the result. Keywords: Green’s function, nonlinear boundary value problems, three-point boundary conditions, existence and uniqueness of solutions.

Pure mathematicsthree-point boundary conditionsValue (computer science)010103 numerical & computational mathematicsFunction (mathematics)Green’s function01 natural sciences010101 applied mathematicsThird ordersymbols.namesakeexistence and uniqueness of solutionsModeling and SimulationGreen's functionsymbolsQA1-939nonlinear boundary value problemsOrder (group theory)Nonlinear boundary value problemBoundary value problemUniqueness0101 mathematicsAnalysisMathematicsMathematicsMathematical Modelling and Analysis
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A theoretical study of the low-lying excited states of thieno[3,4-b]pyrazine

2009

The low-lying electronic excited states of thieno[3,4-b]pyrazine have been studied using the multiconfigurational second-order perturbation CASPT2 theory with extended atomic natural orbital basis sets. The CASPT2 results allow for a full interpretation of the electronic absorption and emission spectra and provide valuable information for the rationalization of the experimental data. The nature, position, and intensity of the spectral bands have been analyzed in detail. A preliminary comparative study of the ground-state geometry of thieno[3,4-b]pyrazine has been performed at the coupled cluster single and doubles and density functional theory levels using a variety of correlation-consisten…

PyrazineOrganic compounds perturbation theoryUNESCO::FÍSICAGeneral Physics and AstronomySpectral bandsRydberg statesFluorescenceGround statesCoupled cluster calculations ; Density functional theory ; Fluorescence ; Ground states ; Organic compounds perturbation theory ; Rydberg stateschemistry.chemical_compoundCoupled clusterchemistryCoupled cluster calculations:FÍSICA [UNESCO]Excited stateDensity functional theoryMoietyDensity functional theoryEmission spectrumPhysical and Theoretical ChemistryAtomic physicsGround state
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Existence of a unique solution for a third-order boundary value problem with nonlocal conditions of integral type

2021

The existence of a unique solution for a third-order boundary value problem with integral condition is proved in several ways. The main tools in the proofs are the Banach fixed point theorem and the Rus’s fixed point theorem. To compare the applicability of the obtained results, some examples are considered.

QA299.6-433Pure mathematicsintegral boundary conditionsBanach fixed point theoremBanach fixed-point theoremApplied MathematicsFixed-point theoremthird-order nonlinear boundary value problemsGreen’s functionType (model theory)Mathematical proofRus’s fixed point theoremThird ordersymbols.namesakeexistence and uniqueness of solutionsGreen's functionsymbolsBoundary value problemAnalysisMathematicsNonlinear Analysis: Modelling and Control
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Stochastic response of MDOF wind-excited structures by means of Volterra series approach

1998

Abstract The role played by the quadratic term of the forcing function in the response statistics of multi-degree-of-freedom (MDOF) wind-excited linear-elastic structures is investigated. This is accomplished by modeling the structural response as a Volterra series up to the second order and neglecting the wind-structure interaction. In order to reduce the computational effort due to the calculation of a large number of multiple integrals, required by the used approach, a recent model of the wind stochastic field is adopted.

Quadratic equationStochastic fieldForce functionControl theoryRenewable Energy Sustainability and the EnvironmentExcited stateMultiple integralMechanical EngineeringVolterra seriesApplied mathematicsMathematicsTerm (time)Civil and Structural Engineering
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Relaxation of Quasilinear Elliptic SystemsviaA-quasiconvex Envelopes

2002

We consider the weak closure WZof the set Z of all feasible pairs (solution, flow) of the family of potential elliptic systems div s0 s=1 s(x)F 0 s(ru(x )+ g(x)) f(x) =0i n; u =( u1;:::;um)2 H 1 0 (; R m ) ; =( 1;:::;s 0 )2 S; where R n is a bounded Lipschitz domain, Fs are strictly convex smooth functions with quadratic growth and S =f measurable j s(x )=0o r 1 ;s =1 ;:::;s0 ;1(x )+ +s0 (x )=1 g .W e show that WZis the zero level set for an integral functional with the integrand QF being the A-quasiconvex envelope for a certain functionF and the operator A = (curl,div) m . If the functions Fs are isotropic, then on the characteristic cone (dened by the operator A) QF coincides with the A-p…

Quadratic growthCurl (mathematics)Pure mathematicsControl and OptimizationElliptic systemsIsotropyMathematical analysisComputational MathematicsQuasiconvex functionLipschitz domainControl and Systems EngineeringBounded functionConvex functionMathematicsESAIM: Control, Optimisation and Calculus of Variations
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Comments on `A new efficient method for calculating perturbation energies using functions which are not quadratically integrable'

1996

The recently proposed method of calculating perturbation energies using a non-normalizable wavefunction by Skala and Cizek is analysed and rigorously proved.

Quadratic growthGeneral Relativity and Quantum CosmologyClassical mechanicsIntegrable systemGeneral Physics and AstronomyPerturbation (astronomy)Statistical and Nonlinear PhysicsWave functionMathematical PhysicsMathematicsJournal of Physics A: Mathematical and General
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