Search results for "Fiber bundle"

showing 10 items of 51 documents

Meson baryon components in the states of the baryon decuplet

2013

We apply an extension of the Weinberg compositeness condition on partial waves of $L=1$ and resonant states to determine the weight of meson-baryon component in the $\Delta(1232)$ resonance and the other members of the $J^P= \frac{3}{2}^+$ baryon decuplet. We obtain an appreciable weight of $\pi N$ in the $\Delta(1232)$ wave function, of the order of 60 \%, which looks more natural when one recalls that experiments on deep inelastic and Drell Yan give a fraction of $\pi N$ component of 34 \% for the nucleon. We also show that, as we go to higher energies in the members of the decuplet, the weights of meson-baryon component decrease and they already show a dominant part for a genuine, non me…

PhysicsParticle physicsMeson010308 nuclear & particles physicsPhysicsQC1-999Nuclear TheoryHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesFunction (mathematics)Resonance (particle physics)01 natural sciencesSection (fiber bundle)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNucleonWave functionNuclear Experiment010306 general physicsEPJ Web of Conferences
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A Closer Study of the Framed Standard Model Yielding Testable New Physics plus a Hidden Sector with Dark Matter Candidates

2018

This closer study of the FSM: [I] retains the earlier results in offering explanation for the existence of three fermion generations, as well as the hierarchical mass and mixing patterns of leptons and quarks; [II] predicts a vector boson $G$ with mass of order TeV which mixes with $\gamma$ and $Z$ of the standard model. The subsequent deviations from the standard mixing scheme are calculable in terms of the $G$ mass. While these deviations for (i) $m_Z - m_W$, (ii) $\Gamma(Z \rightarrow \ell^+ \ell^-)$, and (iii) $\Gamma(Z \rightarrow {\rm hadrons})$ are all within present experimental errors so long as $m_G > 1$ TeV, they should soon be detectable if the $G$ mass is not too much bigger; […

PhysicsQuarkNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstronomy and Astrophysics01 natural sciencesAtomic and Molecular Physics and OpticsStandard ModelVector bosonSection (fiber bundle)Hidden sectorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs boson010306 general physics
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𝔸1-contractibility of affine modifications

2019

We introduce Koras–Russell fiber bundles over algebraically closed fields of characteristic zero. After a single suspension, this exhibits an infinite family of smooth affine [Formula: see text]-contractible [Formula: see text]-folds. Moreover, we give examples of stably [Formula: see text]-contractible smooth affine [Formula: see text]-folds containing a Brieskorn–Pham surface, and a family of smooth affine [Formula: see text]-folds with a higher-dimensional [Formula: see text]-contractible total space.

Pure mathematicsComputer Science::Information RetrievalGeneral Mathematics010102 general mathematicsAstrophysics::Instrumentation and Methods for AstrophysicsZero (complex analysis)Computer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)01 natural sciencesSuspension (topology)Motivic cohomology0103 physical sciencesComputer Science::General LiteratureFiber bundle010307 mathematical physicsAffine transformation0101 mathematicsAlgebraically closed fieldMathematicsInternational Journal of Mathematics
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Discretization of harmonic measures for foliated bundles

2012

We prove in this note that there is, for some foliated bundles, a bijective correspondance between Garnett's harmonic measures and measures on the fiber that are stationary for some probability measure on the holonomy group. As a consequence, we show the uniqueness of the harmonic measure in the case of some foliations transverse to projective fiber bundles.

Pure mathematicsFiber (mathematics)HolonomyPhysics::OpticsHarmonic (mathematics)Dynamical Systems (math.DS)General MedicineHarmonic measureFOS: MathematicsBijectionFiber bundleMathematics::Differential GeometryUniquenessMathematics - Dynamical SystemsMathematics::Symplectic GeometryMathematicsProbability measureComptes Rendus Mathematique
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The first Chevalley–Eilenberg Cohomology group of the Lie algebra on the transverse bundle of a decreasing family of foliations

2010

Abstract In [L. Lebtahi, Lie algebra on the transverse bundle of a decreasing family of foliations, J. Geom. Phys. 60 (2010), 122–133], we defined the transverse bundle V k to a decreasing family of k foliations F i on a manifold M . We have shown that there exists a ( 1 , 1 ) tensor J of V k such that J k ≠ 0 , J k + 1 = 0 and we defined by L J ( V k ) the Lie Algebra of vector fields X on V k such that, for each vector field Y on V k , [ X , J Y ] = J [ X , Y ] . In this note, we study the first Chevalley–Eilenberg Cohomology Group, i.e. the quotient space of derivations of L J ( V k ) by the subspace of inner derivations, denoted by H 1 ( L J ( V k ) ) .

Pure mathematicsFoliacions (Matemàtica)Group (mathematics)General Physics and AstronomyLie Àlgebres deQuotient space (linear algebra)CohomologyAlgebraTensor (intrinsic definition)Lie bracket of vector fieldsLie algebraVector fieldFiber bundleGeometry and TopologyMathematical PhysicsMathematicsJournal of Geometry and Physics
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On the Energy of Distributions, with Application to the Quaternionic Hopf Fibrations

2001

The energy of an oriented q-distribution ? in a compact oriented manifold M is defined to be the energy of the section of the Grassmannian manifold of oriented q-planes in M induced by ?. In the Grassmannian, the Sasaki metric is considered. We show here a condition for a distribution to be a critical point of the energy functional. In the spheres, we see that Hopf fibrations \(\) are critical points. Later, we prove the instability for these fibrations.

Pure mathematicsGeneral MathematicsMathematical analysisCritical point (mathematics)law.inventionSection (fiber bundle)Mathematics::Algebraic GeometrylawGrassmannianSPHERESMathematics::Differential GeometryMathematics::Symplectic GeometryManifold (fluid mechanics)Energy (signal processing)Distribution (differential geometry)Energy functionalMathematicsMonatshefte für Mathematik
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L p-Spaces and the Radon–Nikodym Theorem

2020

In this chapter, we study the spaces of functions whose pth power is integrable. In Section 7.2, we first derive some of the important inequalities (Holder, Minkowski, Jensen) and then in Section 7.3 investigate the case p=2 in more detail.

Radon–Nikodym theoremSection (fiber bundle)symbols.namesakePure mathematicsIntegrable systemMinkowski spaceHilbert spacesymbolsMathematicsNormed vector space
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Applications to Algebraic Cycles: Nori's Theorem

2017

Deligne cohomology is a tool that makes it possible to unify the study of cycles through an object that classifies extensions of ( p , p )-cycles by points in the p -th intermediate Jacobian (which is the target of the Abel–Jacobi map on cycles of codimension p ). This is treated in Section 10.1 with applications to normal functions. Before giving the proof of Nori's theorem in Section 10.6, we need some results from mixed Hodge theory. These are proven in Section 10.2 where we also state different variants of the theorem. Sections 10.3 and 10.4 treat a localto- global principle and an extension of the method of Jacobian representations of cohomology which are both essential for the proof. …

Section (fiber bundle)Algebraic cycleDiscrete mathematicsDeligne cohomologyPure mathematicsMathematics::Algebraic GeometryIntermediate JacobianMathematics::K-Theory and HomologyGroup (mathematics)Hodge theorySheafCohomologyMathematics
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Optional Sampling Theorems

2020

In Chapter 9 we saw that martingales are transformed into martingales if we apply certain admissible gambling strategies. In this chapter, we establish a similar stability property for martingales that are stopped at a random time (optional sampling and optional stopping). In order also to obtain these results for submartingales and supermartingales, in the first section, we start with a decomposition theorem for adapted processes. We show the optional sampling and optional stopping theorems in the second section. The chapter finishes with the investigation of random stopping times with an infinite time horizon.

Section (fiber bundle)Applied mathematicsSampling (statistics)Time horizonOptional stopping theoremStability (probability)MathematicsDecomposition theorem
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Well-behaved *-Representations

2002

This chapter is devoted to the study of the so-called well-behaved *-representations of (partial) *-algebras. Actually one may define are two notions of well-behavedness and we will discuss the relation between them. These notions are introduced in order to avoid pathologies which may arise for general *-representations and to select “nice” representations, which may have a richer theory. In Section 8.1, we construct a class {π p } of *-representations, starting from an unbounded C*-seminorm p and we define nice *-representations in {π p }, called well-behaved. We also characterize their existence. In Section 8.2, we introduce the well-behaved *-representations associated with a compatible …

Section (fiber bundle)Class (set theory)symbols.namesakePure mathematicsHilbert spacesymbolsOrder (ring theory)Linear spanApproximate identityAction (physics)Maximal elementMathematics
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