Search results for "Counterexample"

showing 10 items of 48 documents

COMPUTER SIMULATION OF PROFILES OF INTERFACES BETWEEN COEXISTING PHASES: DO WE UNDERSTAND THEIR FINITE SIZE EFFECTS?

2000

Interfaces between coexisting phases are very common in condensed matter physics, and thus many simulations attempt to characterize their properties, in particular, the interfacial tension and the interfacial profile. However, while theory usually deals with the "intrinsic profile", the latter is not a straightforward output of a simulation: The actual profile (observed in simulations and/or experiments!) is broadened by lateral fluctuations. Therefore, in the usual simulation geometry of L × L × L (in three dimensions), where one chooses suitable boundary conditions to stabilize one or two interfaces of (minimal) area L × L, the profile (and in particular the interfacial width) depends on…

PhysicsCapillary waveMonte Carlo methodGeneral Physics and AstronomyBinary numberStatistical and Nonlinear PhysicsComputer Science ApplicationsSurface tensionRange (mathematics)Computational Theory and MathematicsPerpendicularBoundary value problemStatistical physicsMathematical PhysicsCounterexampleInternational Journal of Modern Physics C
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A holographic approach to low-energy weak interactions of hadrons

2011

We apply the double-trace formalism to incorporate nonleptonic weak interactions of hadrons into holographic models of the strong interactions. We focus our attention upon $\Delta S=1$ nonleptonic kaon decays. By working with a Yang-Mills--Chern-Simons 5-dimensional action, we explicitly show how, at low energies, one recovers the $\Delta S=1$ weak chiral Lagrangian for both the anomalous and nonanomalous sectors. We provide definite predictions for the low energy coefficients in terms of the AdS metric and argue that the double-trace formalism is a 5-dimensional avatar of the Weak Deformation Model introduced long ago by Ecker et al. As a significant phenomenological application, we reasse…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonmesoniinterazioni deboliHolographyFOS: Physical scienceslaw.inventionmodelli olograficisymbols.namesakeAdS/CFT correspondenceTheoretical physicsHigh Energy Physics - PhenomenologyLow energyHigh Energy Physics - Phenomenology (hep-ph)FactorizationlawsymbolsEffective actionLagrangianCounterexample
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Supersymmetry does not imply mass degeneracy

2004

Abstract It is commonly believed that unbroken supersymmetry (SUSY) implies that all members of a supermultiplet have the same mass. We demonstrate that this is not true, by exhibiting a simple counterexample. We employ the formalism of homeotic fermions, in a simple model where CPT conjugate fermions have different masses. This model can be supersymmetrized to a hypermultiplet of fields which form a representation of the conventional N=2 SUSY algebra. Nevertheless, CPT conjugate states in this hypermultiplet have different masses. These surprising results do not violate either the CPT theorem or the Haag–Lopuszanski–Sohnius theorem.

PhysicsParticle physicsNuclear and High Energy PhysicsCPT symmetryHypermultipletHigh Energy Physics::PhenomenologyFísicaSupersymmetryFermionTheoretical physicsFormalism (philosophy of mathematics)High Energy Physics::TheorySupermultipletHigh Energy Physics::ExperimentCounterexampleSupersymmetry algebraPhysics Letters B
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ON A QUESTION OF BEIDLEMAN AND ROBINSON

2002

[EN] In [J. C. Beidleman, D. J. S. Robinson, J. Algebra 1997, 191, 686--703, Theorem A], Beidleman and Robinson proved that if a group satisfies the permutizer condition, it is soluble, its chief factors have order a prime number or 4 and G induces the full group of automorphisms in the chief factors of order 4. In this paper, we show that the converse of this theorem is false by showing some counterexamples. We also find some sufficient conditions for a group satisfying the converse of that theorem to satisfy the permutizer condition.

Pure mathematicsAlgebra and Number TheoryFinite soluble groupGroup (mathematics)Permutizer conditionPrime numberGrups Teoria deAutomorphismCombinatoricsConverseChief factorOrder (group theory)ÀlgebraAlgebra over a fieldMATEMATICA APLICADAMathematicsCounterexampleCommunications in Algebra
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A note on finite determinacy for corank 2 map germs from surfaces to 3-space

2008

AbstractWe study properties of finitely determined corank 2 quasihomogeneous map germs f:($\C^2$, 0) → ($\C^3$, 0). Examples and counter examples of such map germs are presented.

Pure mathematicsDeterminacyGeneral MathematicsCalculusSpace (mathematics)MathematicsCounterexampleMathematical Proceedings of the Cambridge Philosophical Society
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On the quasi-isometric and bi-Lipschitz classification of 3D Riemannian Lie groups.

2021

AbstractThis note is concerned with the geometric classification of connected Lie groups of dimension three or less, endowed with left-invariant Riemannian metrics. On the one hand, assembling results from the literature, we give a review of the complete classification of such groups up to quasi-isometries and we compare the quasi-isometric classification with the bi-Lipschitz classification. On the other hand, we study the problem whether two quasi-isometrically equivalent Lie groups may be made isometric if equipped with suitable left-invariant Riemannian metrics. We show that this is the case for three-dimensional simply connected groups, but it is not true in general for multiply connec…

Pure mathematicsDimension (graph theory)Quasi-isometricisometric53C2301 natural sciencesdifferentiaaligeometria0103 physical sciencesSimply connected spaceMathematics::Metric Geometry0101 mathematicsIsometric20F65bi-LipschitzMathematicsTransitive relationOriginal PaperLie groupsRiemannian manifold010102 general mathematics22D05ryhmäteoriaLie groupBi-Lipschitz; Classification; Isometric; Lie groups; Quasi-isometric; Riemannian manifoldRiemannian manifoldLipschitz continuityClassificationmetriset avaruudetquasi-isometricBi-LipschitzclassificationDifferential geometrygeometria010307 mathematical physicsGeometry and TopologyMathematics::Differential GeometryCounterexampleGeometriae dedicata
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Hitchhiker's guide to the fractional Sobolev spaces

2012

AbstractThis paper deals with the fractional Sobolev spaces Ws,p. We analyze the relations among some of their possible definitions and their role in the trace theory. We prove continuous and compact embeddings, investigating the problem of the extension domains and other regularity results.Most of the results we present here are probably well known to the experts, but we believe that our proofs are original and we do not make use of any interpolation techniques nor pass through the theory of Besov spaces. We also present some counterexamples in non-Lipschitz domains.

Pure mathematicsMathematics(all)General MathematicsMathematical proof01 natural sciencesSobolev inequalityFractional LaplacianSobolev embeddingsMathematics - Analysis of PDEsSettore MAT/05 - Analisi MatematicaFOS: Mathematics0101 mathematicsNehari manifoldMathematicsSobolev spaces for planar domains010102 general mathematicsMathematical analysisFractional Sobolev spacesFractional Sobolev spaces; Gagliardo norm; Fractional Laplacian; Nonlocal energy; Sobolev embeddingsGagliardo normNonlocal energyFunctional Analysis (math.FA)Mathematics - Functional Analysis010101 applied mathematicsSobolev spaceInterpolation spaceAnalysis of PDEs (math.AP)CounterexampleTrace theoryBull. Sci. Math.
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Orbit spaces of Small Tori

2003

Consider an algebraic torus of small dimension acting on an open subset of ℂn, or more generally on a quasiaffine variety such that a separated orbit space exists. We discuss under which conditions this orbit space is quasiprojective. One of our counterexamples provides a toric variety with enough effective invariant Cartier divisors that is not embeddable into a smooth toric variety.

Pure mathematicsMathematics::Commutative AlgebraApplied MathematicsMathematical analysisToric varietyTorusAlgebraic geometryMathematics::Algebraic GeometryMathematics (miscellaneous)Algebraic torusInvariant (mathematics)Mathematics::Symplectic GeometryMathematicsCounterexampleResults in Mathematics
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Multifunctions determined by integrable functions

2019

Integral properties of multifunctions determined by vector valued functions are presented. Such multifunctions quite often serve as examples and counterexamples. In particular it can be observed that the properties of being integrable in the sense of Bochner, McShane or Birkhoff can be transferred to the generated multifunction while Henstock integrability does not guarantee it.

Pure mathematicsPositive multifunctionIntegrable systemApplied Mathematicsselection02 engineering and technologymultifunction determined by a functionTheoretical Computer ScienceFunctional Analysis (math.FA)28B20 26E25 26A39 28B05 46G10 54C60 54C65Mathematics - Functional AnalysisPositive multifunction gauge integral selection multifunction determined by a function measure theory.measure theorySettore MAT/05 - Analisi MatematicaArtificial Intelligence020204 information systemsgauge integral0202 electrical engineering electronic engineering information engineeringFOS: Mathematics020201 artificial intelligence & image processingVector-valued functionSoftwareCounterexampleMathematics
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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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