Search results for "Names"

showing 10 items of 6843 documents

A note on k-generalized projections

2007

Abstract In this note, we investigate characterizations for k -generalized projections (i.e., A k  =  A ∗ ) on Hilbert spaces. The obtained results generalize those for generalized projections on Hilbert spaces in [Hong-Ke Du, Yuan Li, The spectral characterization of generalized projections, Linear Algebra Appl. 400 (2005) 313–318] and those for matrices in [J. Benitez, N. Thome, Characterizations and linear combinations of k -generalized projectors, Linear Algebra Appl. 410 (2005) 150–159].

Pure mathematicsNumerical AnalysisAlgebra and Number TheoryNormal matricesHilbert spaceCharacterization (mathematics)Matrius (Matemàtica)Normal matrixAlgebrasymbols.namesakeLinear algebrasymbolsDiscrete Mathematics and CombinatoricsSpectral projectionGeometry and TopologyÀlgebra linealLinear combinationProjectionst-Potent matricesMathematicsLinear Algebra and its Applications
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OMA: From Research to Engineering Applications

2021

Ambient vibration modal identification, also known as Operational Modal Analysis (OMA), aims to identify the modal properties of a structure based on vibration data collected when the structure is under its operating conditions, i.e., when there is no initial excitation or known artificial excitation. This method for testing and/or monitoring historical buildings and civil structures, is particularly attractive for civil engineers concerned with the safety of complex historical structures. However, in practice, not only records of external force are missing, but uncertainties are involved to a significant extent. Hence, stochastic mechanics approaches are needed in combination with the iden…

Pure mathematicsOrder (ring theory)Context (language use)Operational modal analysisCorrelation function (quantum field theory)Hilbert transformsymbols.namesakeMatrix (mathematics)Operational Modal AnalysisCorrelation functionSingular value decompositionsymbolsModal matrixAnalytical signalHilbert transformSettore ICAR/08 - Scienza Delle CostruzioniStructural identificationMathematics
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Gibbs states, algebraic dynamics and generalized Riesz systems

2020

In PT-quantum mechanics the generator of the dynamics of a physical system is not necessarily a self-adjoint Hamiltonian. It is now clear that this choice does not prevent to get a unitary time evolution and a real spectrum of the Hamiltonian, even if, most of the times, one is forced to deal with biorthogonal sets rather than with on orthonormal basis of eigenvectors. In this paper we consider some extended versions of the Heisenberg algebraic dynamics and we relate this analysis to some generalized version of Gibbs states and to their related KMS-like conditions. We also discuss some preliminary aspects of the Tomita-Takesaki theory in our context.

Pure mathematicsPhysical systemFOS: Physical sciencesBiorthogonal sets of vectors01 natural sciencesUnitary statesymbols.namesakeSettore MAT/05 - Analisi Matematica0103 physical sciencesFOS: MathematicsOrthonormal basis0101 mathematicsAlgebraic numberOperator Algebras (math.OA)Eigenvalues and eigenvectorsMathematical PhysicsMathematics010308 nuclear & particles physicsMathematics::Operator AlgebrasApplied Mathematics010102 general mathematicsTime evolutionMathematics - Operator AlgebrasTomita–Takesaki theoryMathematical Physics (math-ph)Gibbs statesNon-Hermitian HamiltoniansComputational MathematicsComputational Theory and MathematicsBiorthogonal systemsymbolsHamiltonian (quantum mechanics)
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Nonexistence of global weak solutions for a nonlinear Schrodinger equation in an exterior domain

2020

We study the large-time behavior of solutions to the nonlinear exterior problem L u ( t , x ) = &kappa

Pure mathematicsPhysics and Astronomy (miscellaneous)General MathematicsGlobal weak solution01 natural sciencesDomain (mathematical analysis)symbols.namesakeSettore MAT/05 - Analisi MatematicaComputer Science (miscellaneous)Neumann boundary conditionNonlinear Schrödinger equationBall (mathematics)0101 mathematicsNonlinear Schrödinger equationPhysicsComplex-valued functionOpen unitOperator (physics)lcsh:Mathematics010102 general mathematicsUnit normal vectorlcsh:QA1-939010101 applied mathematicsMathematics::LogicChemistry (miscellaneous)symbolsExterior domainNonhomegeneous Neumann boundary condition
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Cohomology, central extensions, and (dynamical) groups

1985

We analyze in this paper the process of group contraction which allows the transition from the Einstenian quantum dynamics to the Galilean one in terms of the cohomology of the Poincare and Galilei groups. It is shown that the cohomological constructions on both groups do not commute with the contraction process. As a result, the extension coboundaries of the Poincare group which lead to extension cocycles of the Galilei group in the “nonrelativistic” limit are characterized geometrically. Finally, the above results are applied to a quantization procedure based on a group manifold.

Pure mathematicsPhysics and Astronomy (miscellaneous)General MathematicsQuantum dynamicsGroup contractionCohomologyGalileansymbols.namesakeMathematics::Quantum AlgebraPoincaré groupPoincaré conjectureCalculussymbolsContraction (operator theory)MathematicsInternational Journal of Theoretical Physics
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A note on zeroes of real polynomials in $C(K)$ spaces

2008

For real C(K) spaces, we show that being injected in a Hilbert space is a 3-space property. As a consequence, we obtain that, when K does not carry a strictly positive Radon measure, every quadratic continuous homogeneous real-valued polynomial on C(K) admits a linear zero subspace enjoying a property which implies non-separability.

Pure mathematicsPolynomialZero setApplied MathematicsGeneral MathematicsCarry (arithmetic)Mathematical analysisZero (complex analysis)Hilbert spacesymbols.namesakeQuadratic equationRadon measuresymbolsSubspace topologyMathematicsProceedings of the American Mathematical Society
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Equivalence of viscosity and weak solutions for the $p(x)$-Laplacian

2010

We consider different notions of solutions to the $p(x)$-Laplace equation $-\div(\abs{Du(x)}^{p(x)-2}Du(x))=0$ with $ 1<p(x)<\infty$. We show by proving a comparison principle that viscosity supersolutions and $p(x)$-superharmonic functions of nonlinear potential theory coincide. This implies that weak and viscosity solutions are the same class of functions, and that viscosity solutions to Dirichlet problems are unique. As an application, we prove a Rad\'o type removability theorem.

Pure mathematicsPrimary 35J92 Secondary 35D40 31C45 35B60Applied MathematicsMathematics::Analysis of PDEsDirichlet distributionPotential theoryNonlinear systemsymbols.namesakeMathematics - Analysis of PDEsFOS: MathematicssymbolsLaplace operatorEquivalence (measure theory)Mathematical PhysicsAnalysisAnalysis of PDEs (math.AP)MathematicsAnnales de l'Institut Henri Poincaré C, Analyse non linéaire
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The Choquet and Kellogg properties for the fine topology when $p=1$ in metric spaces

2017

In the setting of a complete metric space that is equipped with a doubling measure and supports a Poincar´e inequality, we prove the fine Kellogg property, the quasi-Lindel¨of principle, and the Choquet property for the fine topology in the case p = 1. Dans un contexte d’espace m´etrique complet muni d’une mesure doublante et supportant une in´egalit´e de Poincar´e, nous d´emontrons la propri´et´e fine de Kellogg, le quasi-principe de Lindel¨of, et la propri´et´e de Choquet pour la topologie fine dans le cas p = 1. peerReviewed

Pure mathematicsProperty (philosophy)1-fine topologyGeneral MathematicsPoincaré inequalityMathematics::General Topology01 natural sciencesMeasure (mathematics)Complete metric spacefunktioteoriasymbols.namesakeMathematics - Metric GeometryFOS: Mathematics0101 mathematicsMathematicsApplied Mathematics010102 general mathematicsta111Metric Geometry (math.MG)30L99 31E05 26B30function of bounded variationfine Kellogg propertymetriset avaruudet010101 applied mathematicsMetric spacemetric measure spacequasi-Lindelöf principleChoquet propertysymbolspotentiaaliteoriaFine topology
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Remarks about the Besicovitch Covering Property in Carnot groups of step 3 and higher

2016

International audience

Pure mathematicsProperty (philosophy)Applied MathematicsGeneral Mathematicsta111010102 general mathematics[MATH.MATH-CA]Mathematics [math]/Classical Analysis and ODEs [math.CA]16. Peace & justiceHomogeneous quasi-distances01 natural sciencesCarnot groups; Covering theorems; Homogeneous quasi-distances; Mathematics (all); Applied Mathematics010305 fluids & plasmasCombinatoricssymbols.namesakeCarnot groupsCovering theorems0103 physical sciencessymbolsMathematics (all)[MATH]Mathematics [math]0101 mathematicsCarnot cycle[MATH.MATH-MG]Mathematics [math]/Metric Geometry [math.MG]ComputingMilieux_MISCELLANEOUSMathematicsProceedings of the American Mathematical Society
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Nowhere differentiable intrinsic Lipschitz graphs

2021

We construct intrinsic Lipschitz graphs in Carnot groups with the property that, at every point, there exist infinitely many different blow-up limits, none of which is a homogeneous subgroup. This provides counterexamples to a Rademacher theorem for intrinsic Lipschitz graphs.

Pure mathematicsProperty (philosophy)General MathematicsMathematics::Analysis of PDEs01 natural sciencesdifferentiaaligeometriasymbols.namesakeMathematics - Metric Geometry0103 physical sciencesClassical Analysis and ODEs (math.CA)FOS: MathematicsMathematics::Metric GeometryPoint (geometry)Differentiable function0101 mathematicsMathematics010102 general mathematicsryhmäteoriaMetric Geometry (math.MG)16. Peace & justiceLipschitz continuity53C17 58C20 22E25Mathematics - Classical Analysis and ODEsHomogeneoussymbols010307 mathematical physicsCarnot cycleCounterexample
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