Search results for "Vector"

showing 10 items of 2660 documents

Baryon Resonances

2010

10th International Conference on Hypernuclear and Strange Particle Physics. Tokai, JAPAN, SEP 14-18, 2009

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHidden gauge formalism for vector meson interactionNuclear TheoryFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsLambda01 natural sciencesDynamically generated resonancesNuclear Theory (nucl-th)0103 physical sciencesChiral dynamicsConnection (algebraic framework)010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceFísicaBaryonPseudoscalarExcited stateHigh Energy Physics::Experiment
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Peripheral transverse densities of the baryon octet from chiral effective field theory and dispersion analysis

2017

The baryon electromagnetic form factors are expressed in terms of two-dimensional densities describing the distribution of charge and magnetization in transverse space at fixed light-front time. We calculate the transverse densities of the spin-1/2 flavor-octet baryons at peripheral distances b = O(M_\pi^{-1}) using methods of relativistic chiral effective field theory (\chi EFT) and dispersion analysis. The densities are represented as dispersive integrals over the imaginary parts of the form factors in the timelike region (spectral functions). The isovector spectral functions on the two-pion cut t > 4 M_\pi^2 are calculated using relativistic \chi EFT including octet and decuplet baryons.…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryIsoscalarHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)PionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesVector meson010306 general physicsNuclear ExperimentPhysicsIsovector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)HyperonForm factor (quantum field theory)BaryonHigh Energy Physics - PhenomenologyQuantum electrodynamicsHigh Energy Physics::Experiment
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The width of the omega meson in the nuclear medium

2013

We evaluate the width of the omega meson in nuclear matter. We consider the free decay mode of the omega into three pions, which is dominated by rho IEuro decay, and replace the rho and pi propagators by their medium-modified ones. We also take into account the quasielastic and inelastic processes induced by a vector-baryon interaction dominated by vector meson exchange, as well as the contributions coming from the mechanism with medium-modified K , propagators. We obtain a substantial increase of the omega width in the medium, reaching a value of 121 +/- 10 MeV at normal nuclear matter density for an omega at rest, which comes mainly from omega N -> pi pi N, omega NN -> pi NN processes ass…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryNuclear TheoryNuclear physicsFOS: Physical sciences7. Clean energy01 natural sciencesOmegaMomentumNuclear Theory (nucl-th)PionChiral perturbation theory0103 physical sciencesMesons (Nuclear physics)Vector mesonMesons (Física nuclear)Nuclear structure010306 general physicsNuclear ExperimentPhysicsEstructura nuclear010308 nuclear & particles physicsPropagatorHeavy-Ion CollisionsFísicaNuclear matterFísica nuclearHigh Energy Physics::ExperimentHidden Local SymmetryBar (unit)
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Strangeness and charm in nuclear matter

2012

The properties of strange (K, (K) over bar and (K) over bar*) and open-charm (D, (D) over bar and D*) mesons in dense matter are studied using a unitary approach in coupled channels for meson-baryon scattering. In the strangeness sector, the interaction with nucleons always comes through vector-meson exchange, which is evaluated by chiral and hidden gauge Lagrangians. For the interaction of charmed mesons with nucleons we extend the SU(3) Weinberg-Tomozawa Lagrangian to incorporate spin-flavor symmetry and implement a suitable flavor symmetry breaking. The in-medium solution for the scattering amplitude accounts for Pauli blocking effects and meson self-energies. On one hand, we obtain the …

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesStrangeness01 natural sciences7. Clean energyNuclear Theory (nucl-th)Nuclear physicsStrange mesonsTransparency ratioHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesVector mesonSymmetry breakingNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDynamically-generated baryon resonancesFísicaNuclear matterOpen charm in matterPseudoscalarBaryonD-mesic nucleiHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNucleon
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Photoproduction of the f2(1270) resonance

2014

We have performed a calculation of the $\gamma p \to \pi^+ \pi^- p$ reaction, where the two pions have been separated in $D$-wave producing the $f_2(1270)$ resonance. We use elements of the local hidden gauge approach that provides the interaction of vector mesons in which the $f_2(1270)$ resonance appears as a $\rho$-$\rho$ molecular state in $L=0$ and spin 2. The vector meson dominance, incorporated in the local hidden gauge approach converts a photon into a $\rho^0$ meson and the other meson connects the photon with the proton. The picture is simple and has no free parameters, since the parameters of the theory have been constrained in the previous study of the vector-vector states. In a…

Nuclear and High Energy PhysicsParticle physicsPhotonMesonNuclear TheoryHigh Energy Physics::LatticeHadronFOS: Physical sciences01 natural sciencesResonance (particle physics)High Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)PionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentSpin-½Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPropagatorFísicaVector meson dominanceHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Study of the f(2)(1270) , f(2)'(1525) , f(0)(1370) and f(0)(1710) in the J/psi radiative decays

2009

In this paper we present an approach to study the radiative decay modes of the J/psi into a photon and one of the tensor mesons f (2)(1270) , f' (2)(1525) , as well as the scalar ones f (0)(1370) and f (0)(1710) . Especially, we compare predictions that emerge from a scheme where the states appear dynamically in the solution of vector meson-vector meson scattering amplitudes to those from a (admittedly naive) quark model. We provide evidence that it might be possible to distinguish amongst the two scenarios, once improved data are available.

Nuclear and High Energy PhysicsParticle physicsPhotonMesonScalar (mathematics)Radiative decayhadronic decay [J/psi(3100)]01 natural sciencesf0(1710)bound state [vector meson]radiative decay [J/psi(3100)]0103 physical sciencesRadiative transferddc:530f0(1370)Tensor010306 general physicsnumerical calculationsdecay modes [J/psi(3100)]Physicsquark modelf2(1525)ratio [width]010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyQuark modelFísicascalar meson3. Good healthScattering amplitudef2(1270)tensor mesonHigh Energy Physics - Phenomenologywidth [J/psi(3100)]High Energy Physics::Experiment
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Exclusive heavy vector meson electroproduction to NLO in collinear factorisation

2021

We compute the exclusive electroproduction, $\gamma^* p \rightarrow V p$, of heavy quarkonia $V$ to NLO in the collinear factorisation scheme, which has been formally proven for this process. The inclusion of an off-shell virtuality $Q^2$ carried by the photon extends the photoproduction phase space of the exclusive heavy quarkonia observable to electroproduction kinematics. This process is relevant for diffractive scattering at HERA and the upcoming EIC, as well as at the proposed LHeC and FCC.

Nuclear and High Energy PhysicsParticle physicsPhotonNuclear TheoryFOS: Physical sciencesQC770-798hiukkasfysiikka01 natural sciences114 Physical sciencesHigh Energy Physics - Phenomenology (hep-ph)FactorizationNuclear and particle physics. Atomic energy. RadioactivityNLO Computations0103 physical sciencesVector mesonNuclear Experiment010306 general physicsPhysics010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyObservableHERAQCD PhenomenologyHigh Energy Physics - PhenomenologyPhase spaceHigh Energy Physics::Experiment
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Search for the standard model Higgs boson in tau lepton final states

2012

We present a search for the standard model Higgs boson in final states with an electron or muon and a hadronically decaying tau lepton in association with zero, one, or two or more jets using data corresponding to an integrated luminosity of up to 7.3 fb^{-1} collected with the D0 detector at the Fermilab Tevatron collider. The analysis is sensitive to Higgs boson production via gluon gluon fusion, associated vector boson production, and vector boson fusion, and to Higgs boson decays to tau lepton pairs or W boson pairs. Observed (expected) limits are set on the ratio of 95% C.L. upper limits on the cross section times branching ratio, relative to those predicted by the Standard Model, of 1…

Nuclear and High Energy PhysicsParticle physicsTevatronFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentVector bosonStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsBosonCondensed Matter::Quantum GasesPhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyScalar bosonExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonHigh Energy Physics::ExperimentLeptonPhysics Letters B
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Charm and hidden charm scalar mesons in the nuclear medium

2009

We study the renormalization of the properties of low-lying charm and hidden charm scalar mesons in a nuclear medium, concretely of the D-s0(2317) and the theoretical hidden charm state X(3700). We find that for the D-s0(2317), with negligible width at zero density, the width becomes about 100 MeV at normal nuclear-matter density, while in the case of the X(3700) the width becomes as large as 200 MeV. We discuss the origin of this new width and trace it to reactions occurring in the nucleus, while offering a guideline for future experiments testing these changes. We also show how those medium modifications will bring valuable information on the nature of the scalar resonances and the mechan…

Nuclear and High Energy PhysicsParticle physicsTrace (linear algebra)Nuclear TheoryMesonNuclear TheoryScalar (mathematics)FOS: Physical sciencesCHIRAL-SYMMETRY RESTORATIONNuclear Theory (nucl-th)RenormalizationUNITARY APPROACHCharm (quantum number)Nuclear ExperimentNN INTERACTIONPhysicsHEAVY MESONSZero (complex analysis)FísicaLOCAL SYMMETRYMULTIQUARK HADRONSNuclear matterGAUGE BOSONPHI-PHOTOPRODUCTIONHigh Energy Physics::ExperimentPI-PI INTERACTIONNucleonVECTOR-MESONSThe European Physical Journal A
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Meson and baryon resonances

2009

6 pages, 1 table.-- PACS nrs.: 13.75.Lb, 14.40.Cs, 12.40.Vv, 12.40.Yx.-- Talk at the 2008 International Conference on Particles And Nuclei (PANIC08, Nov 9-14, 2008, Eilat, Israel).

Nuclear and High Energy PhysicsParticle physicsbaryon resonanceMesonHigh Energy Physics::LatticeBaryon resonancesNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Hadron spectroscopy0103 physical sciencesddc:530Vector meson010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicshadron spectroscopyHigh Energy Physics::PhenomenologyMeson resonancesFísicaVector meson dominancemeson resonancevector mesonBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentUnitary chiral theoryVector mesons
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