Search results for "relativistic"

showing 10 items of 308 documents

A non-relativistic model for the $[cc][\bar{c}\bar{c}]$ tetraquark

2017

We use a non-relativistic model to study the spectroscopy of a tetraquark composed of $[cc][\bar{c}\bar{c}]$ in a diquark-antidiquark configuration. By numerically solving the Schr\"{o}dinger equation with a Cornell-inspired potential, we separate the four-body problem into three two-body problems. Spin-dependent terms (spin-spin, spin-orbit and tensor) are used to describe the splitting structure of the $c\bar{c}$ spectrum and are also extended to the interaction between diquarks. Recent experimental data on charmonium states are used to fix the parameters of the model and a satisfactory description of the spectrum is obtained. We find that the spin-dependent interaction is sizable in the …

QuarkNuclear and High Energy PhysicsParticle physicsinterpretation of experiments: CERN LHC CollcharmoniumsplittingHigh Energy Physics::LatticeFOS: Physical sciencesBELLE01 natural sciencesSchrödinger equationquarksymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)excited state0103 physical sciencesstructureTensor010306 general physicsInstrumentationSpin-½Physics010308 nuclear & particles physicsHigh Energy Physics::Phenomenologymodel: nonrelativisticAstronomy and AstrophysicstetraquarkThree-body problemDiquarkHigh Energy Physics - Phenomenologythree-body problemdiquark[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Excited statesymbolsSchroedinger equationHigh Energy Physics::ExperimentTetraquarkcharmChinese Physics C
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Effect of relativistic kinematics on the stability of multiquarks

2021

We discuss whether the bound nature of multiquark states in quark models could benefit from relativistic effects on the kinetic energy operator. For mesons and baryons, relativistic corrections to the kinetic energy lead to lower energies, and thus call for a retuning of the parameters of the model. For multiquark states, as well as their respective thresholds, a comparison is made of the results obtained with non-relativistic and relativistic kinetic energy. It is found that the binding energy is lower in the relativistic case. In particular, $QQ\bar q\bar q$ tetraquarks with double heavy flavor become stable for a larger ratio of the heavy to light quark masses; and the all-heavy tetraqua…

QuarkParticle physicsMesonBinding energyNuclear TheoryFOS: Physical scienceseffect: relativisticKinetic energymeson01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesheavy quarkStrong Interactions010306 general physicscorrection: relativisticPhysicsenergy: kinetic010308 nuclear & particles physicsBINDING-ENERGYquark model: nonrelativisticHigh Energy Physics::Phenomenologyenergy: operatortetraquarkbinding energyEnergy operatorBaryonbaryonquark: massHigh Energy Physics - Phenomenologykinematics: relativisticmultiquark: stability[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]TetraquarkHigh Energy Physics::ExperimentRelativistic quantum chemistry
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Predictions for multiplicities and flow harmonics in 5.44 TeV Xe+Xe collisions at the CERN Large Hadron Collider

2018

We present the next-to-leading-order event-by-event EKRT model predictions for the centrality dependence of the charged hadron multiplicity in the pseudorapidity interval $|\eta|\le 0.5$, and for the centrality dependence of the charged hadron flow harmonics $v_n\{2\}$ obtained from 2-particle cumulants, in $\sqrt{s_{NN}}=5.44$ TeV Xe+Xe collisions at the CERN Large Hadron Collider. Our prediction for the 0-5 \% central charged multiplicity is $dN_{\rm ch}/d\eta =1218\pm 46$. We also predict $v_n\{2\}$ in Xe+Xe collisions to increase more slowly from central towards peripheral collisions than those in a Pb+Pb system. We find that at $10 \dots 50$\% centralities $v_2\{2\}$ is smaller and $v_…

QuarkParticle physicsNuclear TheoryHadronFOS: Physical scienceshiukkasfysiikka01 natural sciences114 Physical sciencesNuclear physicsENERGYNuclear Theory (nucl-th)GLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBAYESIAN-ANALYSISRapidityNUCLEAR COLLISIONS010306 general physicsNuclear ExperimentPhysicscollective flowta114010308 nuclear & particles physicsparticle and resonance productionHigh Energy Physics::PhenomenologyHIGH-DENSITY QCDQUARKMultiplicity (mathematics)Nuclear matterHigh Energy Physics - PhenomenologyPseudorapidityHigh Energy Physics::ExperimentImpact parameterhydrodynamic modelsCentralityrelativistic heavy-ion collisions
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Electromagnetic form factors of the nucleon in a relativistic quark pair creation model

2001

We study the effects of the | qqq q\bar{q} > component of the hadronic wave function on the description of the electromagnetic structure of the nucleon. Starting with a qqq baryonic wave function which describes the baryonic and mesonic low energy spectrum, the extra q\bar{q} pair is generated through a relativistic version of the 3P_0 model. It is shown that this model leads to a renormalization of the quark mass that allows one to construct a conserved electromagnetic current. We conclude that these dynamical relativistic corrections play an important role in reproducing the Q2 dependence of the electromagnetic form factors at low Q^2.

QuarkParticle physicsNuclear and High Energy PhysicsNuclear TheoryBar (music)HadronNuclear TheoryFOS: Physical sciences01 natural sciencesMeson cloudRenormalizationNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Electromagnetic form factors0103 physical sciences010306 general physicsWave functionNuclear ExperimentPhysicsNonrelativistic quark models010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Spectrum (functional analysis)High Energy Physics::PhenomenologyBaryonHigh Energy Physics - PhenomenologyFísica nuclearNucleon
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Dipole picture and the nonrelativistic expansion

2022

We study exclusive quarkonium production in the dipole picture at next-to-leading order (NLO) accuracy, using the non-relativistic expansion for the quarkonium wavefunction. This process offers one of the best ways to obtain information about gluon distributions at small $x$, in ultraperipheral heavy ion collisions and in deep inelastic scattering. The quarkonium light cone wave functions needed in the dipole picture have typically been available only at tree level, either in phenomenological models or in the nonrelativistic limit. In this paper, we discuss the compatibility of the dipole approach and the non-relativistic expansion and compute NLO relativistic corrections to the quarkonium …

QuarkParticle physicselectron-ion collisionsPhotonNuclear TheoryQC1-999High Energy Physics::LatticeFOS: Physical scienceshiukkasfysiikka114 Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Light cone0103 physical sciences010306 general physicsWave functionNuclear ExperimentPhysics010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyQuarkoniumDeep inelastic scatteringrelativistic heavy-ion collionsGluonHigh Energy Physics - PhenomenologyDipoleHeavy ionHigh Energy Physics::Experimentydinfysiikka
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Extended van Royen-Weisskopf formalism for lepton-antilepton meson decay widths within non-relativistic quark models

2001

The classical van Royen-Weisskopf formula for the decay width of a meson into a lepton-antilepton pair is modified in order to include non-zero quark momentum contributions within the meson as well as relativistic effects. Besides, a phenomenological electromagnetic density for quarks is introduced. The meson wave functions are obtained from two different models: a chiral constituent quark model and a quark potential model including instanton effects. The modified van Royen-Weisskopf formula is found to improve systematically the results for the widths, giving an overall good description of all known decays.

QuarkPhysicsNuclear and High Energy PhysicsInstantonParticle physicsMesonNuclear Theory010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyConstituent quarkFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)Formalism (philosophy of mathematics)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsRelativistic quantum chemistryWave functionLepton
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Deviation from quark number scaling of the anisotropy parameterv2of pions, kaons, and protons inAu+Aucollisions atsNN=200GeV

2012

Measurements of the anisotropy parameter v(2) of identified hadrons (pions, kaons, and protons) as a function of centrality, transverse momentum p(T), and transverse kinetic energy KET at midrapidity (vertical bar eta vertical bar < 0.35) in Au + Au collisions at root s(N N) = 200 GeV are presented. Pions and protons are identified up to p(T) = 6 GeV/c, and kaons up to p(T) = 4 GeV/c, by combining information from time-of-flight and aerogel Cerenkov detectors in the PHENIX Experiment. The scaling of v(2) with the number of valence quarks (n(q)) has been studied in different centrality bins as a function of transverse momentum and transverse kinetic energy. A deviation from previously observ…

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsNuclear TheoryHadronKinetic energy01 natural sciencesNuclear physicsPion0103 physical sciencesHigh Energy Physics::ExperimentImpact parameterNuclear Experiment010306 general physicsAnisotropyRelativistic Heavy Ion ColliderScalingPhysical Review C
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Cold-Nuclear-Matter Effects on Heavy-Quark Production ind+AuCollisions atsNN=200  GeV

2012

The PHENIX experiment has measured electrons and positrons at midrapidity from the decays of hadrons containing charm and bottom quarks produced in d+Au and p+p collisions at sqrt[S(NN)]=200 GeV in the transverse-momentum range 0.85 ≤ p(T)(e) ≤ 8.5 GeV/c. In central d+Au collisions, the nuclear modification factor R(dA) at 1.5<p(T)<5 GeV/c displays evidence of enhancement of these electrons, relative to those produced in p+p collisions, and shows that the mass-dependent Cronin enhancement observed at the Relativistic Heavy Ion Collider extends to the heavy D meson family. A comparison with the neutral-pion data suggests that the difference in cold-nuclear-matter effects on light- and heavy-…

QuarkPhysicsParticle physicsMeson010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::PhenomenologyHadronGeneral Physics and AstronomyElectronNuclear matter01 natural sciences7. Clean energyNuclear physics0103 physical sciencesD mesonHigh Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderPhysical Review Letters
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Cross section and longitudinal single-spin asymmetry AL for forward W±→μ±ν production in polarized p+p collisions at s=510  GeV

2018

We have measured the cross section and single-spin asymmetries from forward W±→μ±ν production in longitudinally polarized p+p collisions at s=510 GeV using the PHENIX detector at the Relativistic Heavy Ion Collider. The cross sections are consistent with previous measurements at this collision energy, while the most forward and backward longitudinal single spin asymmetries provide new insights into the sea quark helicities in the proton. The charge of the W bosons provides a natural flavor separation of the participating partons. © 2018 authors. Published by the American Physical Society.

QuarkPhysicsProton010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyParton01 natural sciences7. Clean energyAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentPHENIX detectorNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderBosonSpin-½media_commonPhysical Review D
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Cold-Nuclear-Matter Effects on Heavy-Quark Production at Forward and Backward Rapidity ind+AuCollisions atsNN=200  GeV

2014

The PHENIX experiment has measured open heavy-flavor production via semileptonic decay over the transverse momentum range 1 < p(T) < 6 GeV/c at forward and backward rapidity (1.4 < vertical bar y vertical bar < 2.0) in d + Au and p + p collisions at root s(NN) = 200 GeV. In central d + Au collisions, relative to the yield in p + p collisions scaled by the number of binary nucleon-nucleon collisions, a suppression is observed at forward rapidity (in the d-going direction) and an enhancement at backward rapidity (in the Au-going direction). Predictions using nuclear-modified-parton-distribution functions, even with additional nuclear-p(T) broadening, cannot simultaneously reproduce the data a…

QuarkSemileptonic decayPhysicsParticle physicsGeneral Physics and AstronomyBinary numberNuclear matterNuclear physicsDeuteriumTransverse momentumHigh Energy Physics::ExperimentRapidityNuclear ExperimentRelativistic Heavy Ion ColliderPhysical Review Letters
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