Search results for "Quark model"

showing 10 items of 207 documents

Multiquark description of the D-sJ(2860) and D-sJ(2700)

2009

Within a theoretical framework that accounts for all open-charm mesons, including the D-0*(2308), the D-sJ*(2317), and the D-sJ(2460), we analyze the structure and explore possible quantum number assignments for the D-sJ(2860) and the D-sJ(2700) mesons reported by BABAR and Belle Collaborations. The open-charm sector is properly described if considered as a combination of conventional quark-antiquark states and four-quark components. All negative parity and 2(+) states can be understood in terms only of q (q) over bar components, however the description of the 0(+) and 1(+) mesons is improved whenever the mixing between two- and four-quark configurations is included. We analyze all possible…

High Energy Physics::PhenomenologyCharm mesonsFísicaHigh Energy Physics::ExperimentCharm-strange mesonsquark models
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MODELING THE TRANSVERSE MOMENTUM DEPENDENT PARTON DISTRIBUTIONS

2010

We review quark model calculations of the transverse momentum dependent parton distributions (TMDs). For the T-even TMDs, we discuss the physical origin of model relations which hold in a large class of quark models. For the T-odd TMDs we review results in a light-cone constituent quark model (CQM) with the final state interaction effects generated via single-gluon exchange mechanism. As phenomenological application, we show the good agreement between results in the light-cone CQM and available experimental data for the Collins asymmetry.

Large classQuarkParticle physicsNuclear TheoryHigh Energy Physics::Latticemedia_common.quotation_subjectFOS: Physical sciencesConstituent quarkParton01 natural sciencesAsymmetryHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Light cone0103 physical sciences010306 general physicsmedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyQuark modelHigh Energy Physics - PhenomenologyTransverse momentumHigh Energy Physics::ExperimentExclusive Reactions at High Momentum Transfer IV
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A quark model study of strong decays ofX(3915)

2017

Strong decays of are analyzed from two quark model descriptions of , a conventional one in terms of the Cornell potential and an unconventional one from a generalized screened potential. We conclude that the experimental suppression of the OZI allowed decay might be explained in both cases due to the momentum dependence of the decay amplitude. However, the experimental significance of the OZI forbidden decay could favor an unconventional description.

MomentumPhysicsNuclear and High Energy PhysicsParticle physicsAmplitude010308 nuclear & particles physicsHigh Energy Physics::Phenomenology0103 physical sciencesQuark modelHigh Energy Physics::Experiment010306 general physics01 natural sciencesJournal of Physics G: Nuclear and Particle Physics
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Diquark correlations in hadron physics: Origin, impact and evidence

2020

The last decade has seen a marked shift in how the internal structure of hadrons is understood. Modern experimental facilities, new theoretical techniques for the continuum bound-state problem and progress with lattice-regularised QCD have provided strong indications that soft quark+quark (diquark) correlations play a crucial role in hadron physics. For example, theory indicates that the appearance of such correlations is a necessary consequence of dynamical chiral symmetry breaking, viz. a corollary of emergent hadronic mass that is responsible for almost all visible mass in the universe; experiment has uncovered signals for such correlations in the flavour-separation of the proton's elect…

Nuclear TheoryHigh Energy Physics::LatticeHadronNuclear Theoryhiukkasfysiikka01 natural sciencesHigh Energy Physics - ExperimentBroad spectrumHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Hadron physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentQuantum chromodynamicsPhysicsDiquark correlationsBaryon spectra and structureHigh Energy Physics - Lattice (hep-lat)symmetry breaking: chiralDyson-Schwinger equationsDiquarkbound statediquark: correlationHigh Energy Physics - PhenomenologyQuark modelsChiral symmetry breakingPhenomenology (particle physics)QuarkNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]diquark correlationsNuclear Theory (nucl-th)High Energy Physics - Latticehadron physics0103 physical sciencesquantum chromodynamics010306 general physicsBaryon spectra and structure; Diquark correlations; Dyson-Schwinger equations; Lattice quantum chromodynamics; Quantum chromodynamics; Quark modelskvarkit010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]hadron spectroscopyHigh Energy Physics::PhenomenologyLattice quantum chromodynamicsform factor: electromagnetic[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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Spectroscopy, lifetime and decay modes of the $T^-_{bb}$ tetraquark

2019

We present the first full-fledged study of the flavor-exotic isoscalar $T_{bb}^-\equiv b b \bar u \bar d$ tetraquark with spin and parity $J^P=1^+$. We report accurate solutions of the four-body problem in a quark model, characterizing the structure of the state as a function of the ratio $M_Q/m_q$ of the heavy to light quark masses. For such a standard constituent model, $T_{bb}^-$ lies approximately 150 MeV below the strong decay threshold $B^-\bar {B^*}^{0}$ and 105 MeV below the electromagnetic decay threshold $B^- \bar B^0 \gamma$. We evaluate the lifetime of $T_{bb}^-$, identifying the promising decay modes where the tetraquark might be looked for in future experiments. Its total deca…

Nuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesspinHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)multiquarkisoscalarquantum chromodynamics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]structureconstituentlifetimequark modelhadron spectroscopyHigh Energy Physics::Phenomenologysemileptonic decayMULTIQUARK HADRONSquark: massHigh Energy Physics - PhenomenologySTATESparitytetraquark: decay modes[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimenttetraquark: wave function
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Observation of orbitally excited B mesons

1995

Experimental evidence for the existence of orbitally excited B meson states is presented in an analysis of the Bπ and B*π distribution of Q = m(B**) - m(B(*)) - m(π) using Z0decay data taken with the DELPHI detector at LEP. The mean Q-value of the decays B**→ B(*)π is measured to be 284 ± 5 (stat.) ± 15 (syst.) MeV/c2, and the Gaussian width of the signal is 79 ± 5 (stat.) ± 8 (syst.) MeV/c2. This signal can be described as a single resonance of mass m = 5732 ± 5 (stat.) ± 20 (syst.) MeV/c2and full width Γ = 145 ± 28 MeV/c2. The observed shape is also consistent with the production of several broad and narrow states as predicted by the quark model and partly observed in the D-…

Nuclear and High Energy PhysicsE+E ANNIHILATIONLUND MONTE-CARLOElectron–positron annihilationDELPHI; B meson; fragmentation; b-jetB meson01 natural sciencesResonance (particle physics)Full widthPartícules (Física nuclear)JET FRAGMENTATIONDECAYSNuclear physicsPHYSICSfragmentation0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B meson010306 general physicsNuclear ExperimentDetectors de radiacióDELPHIPhysics010308 nuclear & particles physicsQuark modelb-jetLARGE ELECTRON POSITRON COLLIDERExcited statePARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::ExperimentLUND MONTE-CARLO; JET FRAGMENTATION; E+E ANNIHILATION; DECAYS; PHYSICSParticle Physics - ExperimentProduction ratePhysics Letters B
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Discrete dark matter

2010

We propose a new motivation for the stability of dark matter (DM). We suggest that the same non-abelian discrete flavor symmetry which accounts for the observed pattern of neutrino oscillations, spontaneously breaks to a Z2 subgroup which renders DM stable. The simplest scheme leads to a scalar doublet DM potentially detectable in nuclear recoil experiments, inverse neutrino mass hierarchy, hence a neutrinoless double beta decay rate accessible to upcoming searches, while reactor angle equal to zero gives no CP violation in neutrino oscillations.

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Scalar (mathematics)Dark matterFOS: Physical sciencesElementary particle01 natural sciencesNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciences010306 general physicsNeutrino oscillationParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsQuark modelHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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Limits on tau lepton-flavor violating decays into three charged leptons

2010

A search for the neutrinoless, lepton-flavor violating decay of the tau lepton into three charged leptons has been performed using an integrated luminosity of 468 fb(-1) collected with the BABAR detector at the PEP-II collider. In all six decay modes considered, the numbers of events found in data are compatible with the background expectations. Upper limits on the branching fractions are set in the range (1.8-3.3) x 10(-8) at 90% confidence level.

Nuclear and High Energy PhysicsParticle physicsElectron–positron annihilationBABARFOS: Physical sciencesElementary particletau: branching ratioelectron positron: annihilationmeson01 natural sciencesPARTICLE PHYSICS; PEP2; BABARHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decaytau: leptonic decay; lepton: flavor: violation; tau: branching ratio; BaBar; background; SLAC PEP Stor; electron positron: annihilation; tau: pair production; final state: (0neutrino); upper limit; tau- --> lepton+ 2lepton-; 10.54: 10.58 GeV-cms quark: angular momentum; positron electron --> quark antiquark; excited state; mesonexcited state0103 physical sciencesPEP2[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]10.54: 10.58 GeV-cms quark: angular momentumpositron electron --> quark antiquark010306 general physicsfinal state: (0neutrino)PACS: 13.35.DxFlavorPhysicstau- --> lepton+ 2lepton-tau: pair productionlepton flavor violationbackground010308 nuclear & particles physicsQuark modelHigh Energy Physics::Phenomenologylepton: flavor: violationParticle physicsFermionBABAR detectorSLAC PEP StorHEPCharged particletau: leptonic decayPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica de partículesExperimentsupper limitLeptonPhysical Review D
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HEAVY HADRON SPECTROSCOPY: A QUARK MODEL PERSPECTIVE

2012

We present recent results of hadron spectroscopy and hadron hadron interaction from the perspective of constituent quark models. We pay special attention to the role played by higher-order hock space components in the hadron spectra and the connection of this extension with the hadron-hadron interaction. The main goal of our description is to obtain a coherent understanding of the low-energy hadron phenomenology without enforcing any particular model, to constrain its characteristics and learn about the low-energy realization of the theory.

Nuclear and High Energy PhysicsParticle physicsMassesNuclear TheoryMesonNuclear TheoryHadronFOS: Physical sciencesGeneral Physics and AstronomyConstituent quarkFock spaceNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Perspective (geometry)Hadron spectroscopyBaryonsNuclear ExperimentQuantum chromodynamicsPhysicsMesonsHigh Energy Physics::PhenomenologyQuark modelSystemsFísicaMolecular-stateBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentPhenomenology (particle physics)Realization (systems)International Journal of Modern Physics E
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Light baryons and their electromagnetic interactions in the covariant constituent quark model

2012

We extend the confined covariant constituent quark model that was previously developed by us for mesons to the baryon sector. In our numerical calculation we use the same values for the constituent quark masses and the infrared cutoff as have been previously used in the meson sector. In a first application we describe the static properties of the proton and neutron, and the $\Lambda$-hyperon (magnetic moments and charge radii) and the behavior of the nucleon form factors at low momentum transfers. We discuss in some detail the conservation of gauge invariance of the electromagnetic transition matrix elements in the presence of a nonlocal coupling of the baryons to the three constituent quar…

Nuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryConstituent quarkDown quarkFOS: Physical sciencesPROTONBottom quarkHigh Energy Physics - Phenomenology (hep-ph)Nuclear ExperimentPhysicsCOMPOSITE PARTICLESELASTIC SCATTERINGPOLARIZATION TRANSFERHigh Energy Physics::PhenomenologyHyperonRELATIVISTIC 3-QUARK MODELMAGNETIC FORM-FACTORDEUTERONBaryonHigh Energy Physics - PhenomenologyQuantum electrodynamicsHEAVY BARYONSUp quarkNEUTRONHigh Energy Physics::ExperimentSQUARED 4-MOMENTUM TRANSFERSNucleon
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