Search results for "Chromodynamics"

showing 10 items of 1030 documents

Lattice QCD study of the $H$ dibaryon using hexaquark and two-baryon interpolators

2019

Physical review / D 99(7), 074505 (2019). doi:10.1103/PhysRevD.99.074505

Particle physicsnucl-thNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryLattice field theoryFOS: Physical scienceshep-latCorrelation function (quantum field theory)530Computer Science::Digital Libraries01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBound stateddc:530010306 general physicsParticle Physics - PhenomenologyQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)hep-phParticle Physics - LatticeLattice QCDRest frameBaryonHigh Energy Physics - PhenomenologyNuclear Physics - TheoryIsospin
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Density distributions in the $B$ meson

2016

We report on a two-flavor lattice QCD study of the axial, charge and matter distributions of the $B$ meson and its first radial excitation. As our framework is the static limit of Heavy Quark Effective Theory (HQET), taking their Fourier transform gives access to several form factors at the kinematical point $q^2=0$. Moreover they provide some useful information on the nature of an excited state, i.e. a radial excitation of a quark-antiquark bound state or a multihadron state.

Particle physicsquark antiquark: bound stateMesonHigh Energy Physics::LatticeFOS: Physical sciencescharge distribution01 natural sciencesfermion: cloverpi: couplingsymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)density: spatial distributionquark: flavor: 2excited state0103 physical sciencesBound stateB meson010306 general physicscharge: axialform factorPhysicsHeavy Quark Effective Theory[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]finite size: effect010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Form factor (quantum field theory)[ PHYS.HLAT ] Physics [physics]/High Energy Physics - Lattice [hep-lat]Charge (physics)Lattice QCDHigh Energy Physics - PhenomenologyFourier transformkinematicsmatter: distribution function[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]bottom mesonExcited statesymbols[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentquark: Wilsonquantum chromodynamics: lattice
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Measurement of the c0 Baryon Lifetime

2018

We report a measurement of the lifetime of the $��_c^0$ baryon using proton-proton collision data at center-of-mass energies of 7 and 8~TeV, corresponding to an integrated luminosity of 3.0 fb$^{-1}$ collected by the LHCb experiment. The sample consists of about 1000 $��_b^-\to��_c^0��^-\bar��_�� X$ signal decays, where the $��_c^0$ baryon is detected in the $pK^-K^-��^+$ final state and $X$ represents possible additional undetected particles in the decay. The $��_c^0$ lifetime is measured to be $��_{��_c^0} = 268\pm24\pm10\pm2$ fs, where the uncertainties are statistical, systematic, and from the uncertainty in the $D^+$ lifetime, respectively. This value is nearly four times larger than, …

Particles and fieldGeneral PhysicsMesonGeneral Physics and AstronomyFOS: Physical sciences01 natural sciences7. Clean energyOmega09 EngineeringNOLuminosityHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)0103 physical sciencesPhysicHeavy baryonTOOLSDG 7 - Affordable and Clean EnergyLHCb - Abteilung Hinton010306 general physicsINCLUSIVE WEAK DECAYS; DISCARDING 1/N(C); RULE; TOOL01 Mathematical SciencesQuantum chromodynamicsPhysics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energy02 Physical Sciences010308 nuclear & particles physicsQuark modelParticle physicsState (functional analysis)HEPDISCARDING 1/N(C)BaryonLHCbHadron colliderHigh Energy Physics::ExperimentINCLUSIVE WEAK DECAYSLHCAtomic physicsFísica de partículesExperimentsRULECharm physics Oscillation Flavor physics Hadron-Hadron scattering
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Isolated photon production in proton-nucleus collisions at forward rapidity

2018

We calculate isolated photon production at forward rapidities in proton-nucleus collisions in the Color Glass Condensate framework. Our calculation uses dipole cross sections solved from the running coupling Balitsky-Kovchegov equation with an initial condition fit to deep inelastic scattering data. For comparison, we also update the results for the nuclear modification factor for pion production in the same kinematics. We present predictions for future forward RHIC and LHC measurements at $\sqrt{s_{NN}}=200$ GeV and $\sqrt{s_{NN}}=8$ TeV.

PhotonNuclear TheoryProton7. Clean energy01 natural sciencesColor-glass condensateHigh Energy Physics - Phenomenology (hep-ph)coupling constant: energy dependenceDEPENDENCEPIONNuclear Experiment[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]Brookhaven RHIC CollPhysicsphoton lepton and quark productionLarge Hadron ColliderD+AU COLLISIONSphotonBalitsky-Kovchegov equationP-PB COLLISIONSHigh Energy Physics - PhenomenologyCERN LHC Colllepton and quark productionLHCphoton: forward production[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencespi: hadroproduction114 Physical sciencesNuclear Theory (nucl-th)Nuclear physicsPiondeep inelastic scatteringquantum chromodynamics0103 physical sciencesRapidity010306 general physicsp nucleus: scatteringta114010308 nuclear & particles physicsCOLOR GLASS CONDENSATEDeep inelastic scatteringHADRON-PRODUCTIONboundary conditionDipolerapidityQCD in nuclear reactions[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]TEV[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]cross section: dipole
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Transverse extension of partons in the proton probed in the sea-quark range by measuring the DVCS cross section

2019

Physics letters / B B793, 188-194 (2019). doi:10.1016/j.physletb.2019.04.038

Photongeneralized parton distributionmuon: polarizationProtonGeneralized Parton DistributionPartonmeasured [cross section]Proton sizenucl-exmomentum transfer dependence01 natural sciencesCOMPASSSubatomär fysikp: sizeSubatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentMonte CarloQuantum chromodynamicsPhysicsRange (particle radiation)photon: productionGeneralized Parton DistributionsCOMPASS; Deep inelastic scattering; Deeply virtual Compton scattering; Exclusive reactions; Generalized Parton Distributions; Proton size; Quantum chromodynamicsExclusive reactionlcsh:QC1-999transversebeam [muon]Exclusive reactionsslopesize: (transverse)Particle Physics - ExperimentDeep inelastic scatteringQuarkNuclear and High Energy Physicsexclusive reactionslope: (calculated)liquid: target [hydrogen]photon: mediation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530Nuclear physicshydrogen: liquid: target0103 physical sciencesddc:530Nuclear Physics - Experiment010306 general physicsbeam: polarizationhep-ex010308 nuclear & particles physicsmuon: beam160 GeV/cmuon p --> muon p photonsize [p]Compton scatteringcross section: measuredCERN SPSDeep inelastic scattering[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentDeeply virtual Compton scatteringlcsh:PhysicsQuantum chromodynamicsexperimental results
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Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at √s = 7 TeV with the ATLAS detector

2011

The inclusive and dijet production cross-sections have been measured for jets containing b-hadrons (b-jets) in proton–proton collisions at a centre-of-mass energy of √s =7 TeV, using the ATLAS detector at the LHC. The measurements use data corresponding to an integrated luminosity of 34 pb[superscript −1]. The b-jets are identified using either a lifetime-based method, where secondary decay vertices of b-hadrons in jets are reconstructed using information from the tracking detectors, or a muon-based method where the presence of a muon is used to identify semileptonic decays of b-hadrons inside jets. The inclusive b-jet cross-section is measured as a function of transverse momentum in the ra…

Physics and Astronomy (miscellaneous)01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massNuclear ExperimentDetectors de radiacióPhysicsQuantum chromodynamicsLarge Hadron ColliderLuminosity (scattering theory)dijet cross-sections; b-jets; pp collisions; ATLAS detectorAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleATLASP(P)Over-Bar Collisionsmedicine.anatomical_structurePhysical SciencesLHCParticle Physics - ExperimentSemileptonic decayParticle physicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineFysikRapidityddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasScience & TechnologyMuonBottom-Quark ProductionATLAS detectorParton Distributions010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicab-jetsHigh Energy Physics::Experimentproton-proton collisionsDecays
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Study of ordered hadron chains with the ATLAS detector

2017

The analysis of the momentum difference between charged hadrons in high-energy proton-proton collisions is performed in order to study coherent particle production. The observed correlation pattern agrees with a model of a helical QCD string fragmenting into a chain of ground-state hadrons. A threshold momentum difference in the production of adjacent pairs of charged hadrons is observed, in agreement with model predictions. The presence of low-mass hadron chains also explains the emergence of charge-combination-dependent two-particle correlations commonly attributed to Bose-Einstein interference. The data sample consists of 190 μb-1 of minimum-bias events collected with proton-proton colli…

Physics and Astronomy (miscellaneous)Atlas detectorHadronNuclear Theory01 natural sciencesangular correlation [charged particle]High Energy Physics - ExperimentSubatomär fysikHigh Energy Physics - Experiment (hep-ex)correlation: Bose-EinsteinSubatomic Physicsscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]difference [momentum]Nuclear ExperimentQCQuantum chromodynamicsPhysicsLarge Hadron ColliderAtlas (topology)Settore FIS/01 - Fisica SperimentaleMonte Carlo [numerical calculations]ATLASCERN LHC Coll7000 GeV-cmsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGangular distribution: measuredLHCcolliding beams [p p]numerical calculations: Monte Carlomeasured [angular distribution]Particle Physics - ExperimentCoherence (physics)correlation: two-particleParticle physicsp p: scatteringCiências Naturais::Ciências Físicas530 Physics:Ciências Físicas [Ciências Naturais]ground state [hadron]interferencequantum chromodynamics: stringFOS: Physical sciences530Nuclear physicsNational Graphene InstituteBose-Einstein [correlation][ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciencesddc:530High Energy Physics010306 general physicstwo-particle [correlation]Ciencias ExactasScience & TechnologyATLAS detector010308 nuclear & particles physicshep-exmomentum: differenceHigh Energy Physics::PhenomenologyFísicacoherencestring [quantum chromodynamics]hadron: ground stateQCD stringResearchInstitutes_Networks_Beacons/national_graphene_instituteExperimental High Energy Physicsproton-proton collisionsHigh Energy Physics::Experimentcharged particle: angular correlationp p: colliding beamsexperimental resultsPhysical Review D
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Charm-quark fragmentation fractions and production cross section at midrapidity in pp collisions at the LHC

2022

Physical review / D 105(1), L011103 (2022). doi:10.1103/PhysRevD.105.L011103

Physics and Astronomy (miscellaneous)electron p: interactionPROTON-PROTON COLLISIONSMESON PRODUCTIONROOT-S=5.02 TEVmeasured [cross section]hiukkasfysiikka2760 GeV-cms/nucleon01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ALICEscattering [p p]ground state [charm]Charm; p-p collisions[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experimentcharm: ground statep-p collisionsMeson productioninteraction [electron p]CERN LHC Coll7000 GeV-cms/nucleonParticle Physics - Experimentperturbation theory [quantum chromodynamics]p p: scatteringCharmcharm: fragmentation ; p p: scattering ; electron p: interaction ; charm: ground state ; quantum chromodynamics: perturbation theory ; cross section: measured ; hadron hadron: interaction ; CERN LHC Coll ; rapidity ; ALICE ; experimental results ; 2760 GeV-cms/nucleon ; 5020 GeV-cms/nucleon ; 7000 GeV-cms/nucleoneducationFOS: Physical sciencesfragmentation [charm][PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530114 Physical sciencesProton-proton collisions0103 physical sciencescharm fragmentation fractions nuclear physicsddc:5305020 GeV-cms/nucleonNuclear Physics - Experimentcharm: fragmentationD-0quantum chromodynamics: perturbation theory010306 general physicshadron hadron: interactionPROTON-PROTON COLLISIONS; MESON PRODUCTION; ROOT-S=5.02 TEV; QCD; D-0interaction [hadron hadron]010308 nuclear & particles physicsHigh Energy Physics::Phenomenologycross section: measuredRoot-s=5.02 tevQCDQcdrapidityHigh Energy Physics::Experimentkvanttiväridynamiikkaexperimental results
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Three-body forces in the quark model

2008

The constituent quark model has been very useful for the description of many physical properties of baryons, achieving in most cases a fair agreement with the experimental data 1 The model is based on a non relativistic QCD-inspired dynamics including a harmonic oscillator (h.o.) confinement potential and a spin dependent (hyperfine) interaction. The use of Lovelace coordinates p, ~ avoides any problem with the center of mass motion, while the h.o. potential provides a simple basis for ana ly t ica l calculations, which is a very important feature for many applications, like the evaluation of form factors and Meson Exchange Currents 2. On the other hand the h.o. spectrum is too degenerate w…

PhysicsBody forceQuantum chromodynamicsBaryonQuarkParticle physicsMesonQuantum electrodynamicsQuark modelConstituent quarkHarmonic oscillator
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η−η′(−glue) Mixing from the Chiral Lagrangian

2010

The η − η ′ mixing from the chiral Lagrangian is reviewed. It is shown how the Feldman-Kroll-Stech ansazt can be derived from the chiral Lagrangian. The inclusion of the glueball is also discussed.

PhysicsChiral anomalyQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryGlueballHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyThermodynamicsElementary particleAtomic and Molecular Physics and OpticsPhysics::Atomic PhysicsQuantum field theoryMathematics::Symplectic GeometryComputer Science::DatabasesMixing (physics)BosonNuclear Physics B - Proceedings Supplements
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