Search results for "Pion"

showing 10 items of 1304 documents

Backward electroproduction ofπ0mesons on protons in the region of nucleon resonances at four momentum transfer squaredQ2=1.0GeV2

2004

Exclusive electroproduction of pi{sup 0} mesons on protons in the backward hemisphere has been studied at Q2 = 1.0 GeV2 by detecting protons in the forward direction in coincidence with scattered electrons from the 4 GeV electron beam in Jefferson Lab's Hall A. The data span the range of the total (gamma*p) center-of-mass energy W from the pion production threshold to W = 2.0 GeV. The differential cross sections sigma{sub T} + epsilon sigma{sub L}, sigma{sub TL}, and sigma{sub TT} were separated from the azimuthal distribution and are presented together with the MAID and SAID parameterizations.

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsNuclear TheoryHadronMomentum transferSigma01 natural sciencesNuclear physicsBaryonPion0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonLeptonPhysical Review C
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Decay of axial-vector mesons into VP andPγ

2004

We propose a phenomenological Lagrangian for the decay of the SU(3) nonets of the axial-vector mesons of J{sup PC}=1{sup +-},1{sup ++} into a vector meson and a pseudoscalar constructed with tensor fields for the vector and axial-vector mesons. The formulation leads to a good reproduction of the different decay branching ratios and assuming vector meson dominance (VMD) it also leads to good results for the radiative decay of the a{sub 1} into pion and photon, and in agreement with the structure proposed in the chiral tensor formulation of radiative decay of axial-vector mesons. The two SU(3) parameters and the mixing angle of K{sub 1A} and K{sub 1B} needed to give the physical K{sub 1}(1270…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonBranching fractionHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyVector meson dominanceTensor fieldNuclear physicsPseudoscalarPionHigh Energy Physics::ExperimentVector mesonPseudovectorPhysical Review D
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Two-meson cloud contribution to the baryon antidecuplet binding

2004

We study the two-meson virtual cloud contribution to the self-energy of the SU(3) antidecuplet, to which the Theta+ pentaquark is assumed to belong. This is motivated by the large branching ratio of the N(1710) decay into two pions and one nucleon. We derive effective Lagrangians that describe the N(1710) decay into N-pi-pi with two pions in s or p wave. We obtain increased binding for all members of the antidecuplet and a contribution to the mass splitting between states with different strangeness which is at least 20 % of the empirical one. We also provide predictions for three-body decays of the pentaquark antidecuplet.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonBranching fractionHigh Energy Physics::LatticeNuclear TheoryQuark modelFOS: Physical sciencesFísicaStrangenessPentaquarkNuclear physicsBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics::ExperimentNuclear ExperimentNucleonPhysical Review C
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Decay of vector-vector resonances into $\gamma$ and a pseudoscalar meson

2010

We study the decay of dynamically generated resonances from the interaction of two vectors into a $\ensuremath{\gamma}$ and a pseudoscalar meson. The dynamics requires anomalous terms involving vertices with two vectors and a pseudoscalar, which renders it special. We compare our result with data on ${K}_{2}^{*+}(1430)\ensuremath{\rightarrow}{K}^{+}\ensuremath{\gamma}$ and ${K}_{2}^{*0}(1430)\ensuremath{\rightarrow}{K}^{0}\ensuremath{\gamma}$ and find a good agreement with the data for the ${K}_{2}^{*+}(1430)$ case and a width considerably smaller than the upper bound measured for the ${K}_{2}^{*0}(1430)$ meson. We also investigate the decay into ${\ensuremath{\pi}}^{+}\ensuremath{\gamma}$ …

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyVertex functionFísicaElementary particlePseudoscalar mesonPseudoscalarParticle decayHigh Energy Physics - PhenomenologyPion
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Quark mean field model for nucleons in nuclei

1998

We propose the quark mean field model for nucleons in nuclei, where the meson mean fields created by other nucleons act on quarks in a nucleon and change the nucleon properties in nuclei. We take the constituent quark model for the nucleon, which naturally allows the direct coupling of pions and in turn other mesons as $\ensuremath{\sigma}$ and $\ensuremath{\omega}$ mesons. We find very good nuclear matter properties with the use of the nonlinear self-energy terms in the meson Lagrangian. We expect the spin-orbit splitting in finite nuclei to be large due to the large reduction of the nucleon mass, which is in agreement with experiment. The nucleon size increases by about 7% at the normal m…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryDown quarkConstituent quarkBottom quarkNuclear physicsStrange matterPionUp quarkHigh Energy Physics::ExperimentNuclear ExperimentNucleonPhysical Review C
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Hidden gauge formalism for the radiative decays of axial-vector mesons

2009

24 pages, 6 tables, 11 figures.--ISI article identifier:000262979700040 .-- ArXiv pre-print avaible at:http://arxiv.org/abs/0809.0943

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPseudoscalar mesonPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics::ExperimentGauge theoryVector mesonPseudovectorGauge symmetry
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Prediction of a $Z_c(4000)$ $D^* \bar D^*$ state and relationship to the claimed $Z_c(4025)$

2014

After discussing the OZI suppression of one light meson exchange in the interaction of $D^* \bar D^*$ with isospin I=1, we study the contribution of two pion exchange to the interaction and the exchange of a heavy vector $J/\psi$. We find this latter mechanism weak but enough to barely bind the system in J=2 with a mass around 4000 MeV, while the effect of the two pion exchange is a net attraction but weaker than that from $J/\psi$ exchange. We discuss this state and try to relate it to the $Z_c(4025)$ state, above the $D^* \bar D^*$ threshold, claimed in an experiment at BES from and enhancement of the $D^* \bar D^*$ distribution close to threshold. Together with the results from a recent …

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesState (functional analysis)High Energy Physics - PhenomenologyDistribution (mathematics)PionHigh Energy Physics - Phenomenology (hep-ph)IsospinHigh Energy Physics::ExperimentNuclear ExperimentBar (unit)
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sigma meson in a nuclear medium through two pion photoproduction

2003

We show theoretical results for $(\gamma, \pi^0 \pi^0)$ production on nucleons and nuclei in the kinematical region where the scalar isoscalar $\pi \pi$ amplitude is influenced by the $\sigma$ pole. The final state interaction of the pions modified by the nuclear medium produces a spectacular shift of strength of the two pion invariant mass distribution induced by the moving of the $\sigma$ pole to lower masses and widths as the nuclear density increases.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonIsoscalarScalar (mathematics)Nuclear TheoryFísicaAmplitudePionInvariant massNucleonNuclear ExperimentNuclear density
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Coherent pion production off nuclei at T2K and MiniBooNE energies revisited

2010

As a result of a new improved fit to old bubble chamber data of the dominant axial C-5(A) nucleon-to-delta form factor, and due to the relevance of this form factor for neutrino induced coherent pion production, we reevaluate our model predictions in [Phys. Rev. D 79, 013002 ( 2009)] for different observables of the latter reaction. Central values for the total cross sections increase by 20%-30%, while differential cross sections do not change their shape appreciably. Furthermore, we also compute the uncertainties on total, differential, and flux-averaged cross sections induced by the errors in the determination of C-5(A). Our new results turn out to be compatible within about 1 sigma with …

PhysicsNuclear and High Energy PhysicsParticle physicsMesonNuclear Theory010308 nuclear & particles physicsHadronForm factor (quantum field theory)FísicaFOS: Physical sciencesElementary particle01 natural sciences7. Clean energyNuclear physicsBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesProduction (computer science)010306 general physicsNucleon
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Sequential vector and axial-vector meson exchange and chiral loops in radiative phi decay

2003

We study the radiative $\phi$ decay into $\pi^0 \pi^0 \gamma$ and $\pi^0 \eta \gamma $ taking into account mechanisms in which there are two sequential vector-vector-pseudoscalar or axial-vector--vector--pseudoscalar steps followed by the coupling of a vector meson to the photon, considering the final state interaction of the two mesons. There are other mechanisms in which two kaons are produced through the same sequential mechanisms or from $\phi$ decay into two kaons and then undergo final state interaction leading to the final pair of pions or $\pi^0 \eta$, this latter mechanism being the leading one. The results of the parameter free theory, together with the theoretical uncertainties, …

PhysicsNuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHadronFOS: Physical sciencesFísicaElementary particleNuclear physicsHigh Energy Physics - PhenomenologyParticle decayHigh Energy Physics - Phenomenology (hep-ph)PionRadiative transferHigh Energy Physics::ExperimentVector mesonNuclear ExperimentPseudovectorNuclear Physics A
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