Search results for "meson"

showing 10 items of 1548 documents

Chiral unitary approach to eta'N scattering at low energies

2010

We study the \eta' N interaction within a chiral unitary approach which includes \pi N, \eta N and related pseudoscalar meson-baryon coupled channels. Since the SU(3) singlet does not contribute to the standard interaction and the \eta' is mostly a singlet, the resulting scattering amplitude is very small and inconsistent with experimental estimations of the \eta' N scattering length. The additional consideration of vector meson-baryon states into the coupled channel scheme, via normal and anomalous couplings of pseudoscalar to vector mesons, enhances substantially the \eta' N amplitude. We also exploit the freedom of adding to the Lagrangian a new term, allowed by the symmetries of QCD, wh…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear Theory01 natural sciencesQuantum mechanics0103 physical sciencesMesons (Nuclear physics)Mesons (Física nuclear)010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsUnitarityReaccions nuclears010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaCromodinàmica quàntica Partícules (Física nuclear)Scattering lengthBaryonPseudoscalarScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNuclear reactionsQuantum chromodynamics
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Scalar spectrum in a graviton soft wall model

2020

In this study we present a unified phenomenological analysis of the scalar glueball and scalar meson spectra within an AdS/QCD framework in the bottom up approach. For this purpose we generalize the recently developed graviton soft-wall (GSW) model, which has shown an excellent agreement with the lattice QCD glueball spectrum, to a description of glueballs and mesons with a unique energy scale. In this scheme, dilatonic effects, are incorporated in the metric as a deformation of the AdS space. We apply the model also to the heavy meson spectra with success. We obtain quadratic mass equations for all scalar mesons while the glueballs satisfy an almost linear mass equation. Besides their spec…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeScalar (mathematics)FOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Spectrum0103 physical sciencesAdS/CFT010306 general physicsScalar mesonQuantum chromodynamicsPhysics010308 nuclear & particles physicsGlueballHigh Energy Physics::PhenomenologyGravitonLattice QCDMesonMass formulaHigh Energy Physics - PhenomenologyGlueballHigh 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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Interaction of vector mesons with baryons and nuclei

2012

After some short introductory remarks on particular issues on the vector mesons in nuclei, in this paper we present a short review of recent developments concerning the interaction of vector mesons with baryons and with nuclei from a modern perspective using the local hidden gauge formalism for the interaction of vector mesons. We present results for the vector baryon interaction and in particular for the resonances which appear as composite states, dynamically generated from the interaction of vector mesons with baryons, taking also the mixing of these states with pseudoscalars and baryons into account. We then venture into the charm sector, reporting on hidden charm baryon states around 4…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryNuclear TheoryNuclear physicsFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesNuclear Theory (nucl-th)0103 physical sciencesBaryonsMesons (Nuclear physics)Mesons (Física nuclear)010306 general physicsNuclear ExperimentBarionsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaBaryonFormalism (philosophy of mathematics)High Energy Physics::ExperimentFísica nuclear
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Nature of the light scalar mesons

2005

Despite the apparent simplicity of meson spectroscopy, light scalar mesons cannot be accommodated in the usual $q\bar q$ structure. We study the description of the scalar mesons below 2 GeV in terms of the mixing of a chiral nonet of tetraquarks with conventional $q\bar q$ states. A strong diquark-antidiquark component is found for several states. The consideration of a glueball as dictated by quenched lattice QCD drives a coherent picture of the isoscalar mesons.

Nuclear and High Energy PhysicsParticle physicsMesonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]IsoscalarHigh Energy Physics::Latticemeson massquark confinementLattice field theoryNuclear TheoryFOS: Physical sciencessparticles01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesquantum chromodynamics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsGlueballHigh Energy Physics::PhenomenologyScalar (physics)lattice field theory12.39.-x 12.38.-tFísicaLattice QCDDiquarkHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentchiral symmetries
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Detecting the long-distance structure of the X(3872)

2014

We study the X(3872)-->D^0 \bar D^0 \pi^0 decay within a D \bar D^* molecular picture for the X(3872) state. This decay mode is more sensitive to the long-distance structure of the X(3872) resonance than its J/\psi\pi\pi and J/\psi3\pi decays, which are mainly controlled by the details of the X(3872) wave function at short distances. We show that the D^0 \bar D^0 final state interaction can be important, and that a precise measurement of this partial decay width can provide valuable information on the interaction strength between the D^{(*)} \bar D^{(*)} charm mesons.

Nuclear and High Energy PhysicsParticle physicsMeson[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th][SDU.ASTR.CO]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO]Structure (category theory)FOS: Physical sciencesInteraction strength01 natural sciencesHigh Energy Physics - Experiment[PHYS.ASTR.CO]Physics [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO]High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsWave functionComputer Science::DatabasesPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentBar (unit)X(3872)
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Charmed hadrons in nuclear medium

2010

5th International Conference on Quarks and Nuclear Physics (QNP09).Inst High Energy Phys Chinese Acad Sci, Beijing, PEOPLES R CHINA, SEP 21-25, 2009

Nuclear and High Energy PhysicsParticle physicsMesondynamically-generated baryonic resonancesNuclear TheoryHadronScalar (mathematics)Nuclear TheoryFOS: Physical sciencesspectral functionCharmed and hidden charmed scalar resonances01 natural sciences7. Clean energyNuclear Theory (nucl-th)symbols.namesakePauli exclusion principleHigh Energy Physics - Phenomenology (hep-ph)charmed and hidden charmed scalar resonances0103 physical sciencesNuclear Experiment (nucl-ex)Open-charm mesons010306 general physicsNuclear ExperimentInstrumentationNuclear ExperimentPhysics010308 nuclear & particles physicsBlocking (radio)Dynamically-generated baryonic resonancesHigh Energy Physics::PhenomenologyFísicaAstronomy and AstrophysicsSpectral functionBaryonHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentDense matterRESONANCESMATTERopen-charm mesons
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Search forCPviolation usingT-odd correlations inD+→K+KS0π+π−andDs+→K+KS0π+π−decays

2010

We search for CP violation in a sample of 20,000 Cabibbo-suppressed decays, $D^+\rightarrow K^+K^0_S\pi^+\pi^-$, and 30,000 Cabibbo-favored decays, $D_s^+\rightarrow K^+K^0_S\pi^+\pi^-$. We use 520 $fb^{-1}$ of data recorded by the BaBar detector at the PEP-II asymmetric-energy $e^+e^-$ collider operating at center of mass energies near 10.6 $GeV$. We search for CP violation in the difference between the $T$-odd asymmetries obtained using triple product correlations of the $D^+$ ($D_s^+$) and $D^-$ ($D_s^-$) decays, respectively. The $T$ violation parameter values obtained are $\mathcal{A}_T(D^+) = (-12.0 \pm 10.0_{stat} \pm 4.6_{syst})\times 10^{-3}$ and $\mathcal{A}_T(D_s^+) = (-13.6 \pm …

Nuclear and High Energy PhysicsParticle physicsMesonmedia_common.quotation_subjectElectron–positron annihilationHadronElementary particle01 natural sciencesAsymmetrylaw.inventionStandard ModelNuclear physicsParticle decayPionlaw0103 physical sciences010306 general physicsCollidermedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTriple productCP violationHigh Energy Physics::ExperimentCenter of massPhysical Review D
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Evidence for an anomalous like-sign dimuon charge asymmetry

2010

We measure the charge asymmetry $A\equiv(N^{++} - N^{--})/(N^{++} + N^{--})$ of like-sign dimuon events in 6.1~fb$^{-1}$ of $p\bar{p}$ collisions recorded with the D0 detector at a center-of-mass energy $\sqrt{s}=1.96$~TeV at the Fermilab Tevatron collider. From $A$ we extract the like-sign dimuon charge asymmetry in semileptonic $b$-hadron decays: $\aslb=-0.00957\pm0.00251\thinspace({\rm stat})\pm0.00146\thinspace({\rm sys})$. It differs by 3.2~standard deviations from the standard model prediction $\aslb({\rm SM})=(-2.3^{+0.5}_{-0.6})\times10^{-4}$, and provides first evidence of anomalous $CP$ violation in the mixing of neutral $B$ mesons.

Nuclear and High Energy PhysicsParticle physicsMesonmedia_common.quotation_subjectHadronTevatronGeneral Physics and AstronomyFOS: Physical sciencesElementary particleAsymmetry01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsParticle decayHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B meson010306 general physicsNuclear Experimentmedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::Phenomenology13.25.Hw; 14.40.Nd3. Good healthCP violationHigh Energy Physics::Experiment
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