Search results for "PARTICLE PHYSICS"

showing 10 items of 6826 documents

Search for new particles decaying into dijets in proton-antiproton collisions at root s=1.96 TeV

2009

We present a search for new particles which produce narrow two-jet (dijet) resonances using proton-antiproton collision data corresponding to an integrated luminosity of 1.13 fb(-1) collected with the CDF II detector. The measured dijet mass spectrum is found to be consistent with next-to-leading-order perturbative QCD predictions, and no significant evidence of new particles is found. We set upper limits at the 95% confidence level on cross sections times the branching fraction for the production of new particles decaying into dijets with both jets having a rapidity magnitude vertical bar y vertical bar < 1. These limits are used to determine the mass exclusions for the excited quark, axig…

QuarkNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesddc:500.2114 Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Rapidity010306 general physics13.85.Rm 14.70.Pw 14.80.-jQuantum chromodynamicsPhysicshep-ex010308 nuclear & particles physicsBranching fractionPhysicsHigh Energy Physics::PhenomenologyPerturbative QCD3. Good healthDiquarkAntiprotonHigh Energy Physics::Experiment
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Pentaquarks with anticharm or beauty revisited

2019

We use a constituent model to analyze the stability of pentaquark $\bar Q qqqq$ configurations with a heavy antiquark $\bar c$ or $\bar b$, and four light quarks $uuds$, $ddsu$ or $ssud$. The interplay between chromoelectric and chromomagnetic effects is not favorable, and, as a consequence, no bound state is found below the lowest dissociation threshold.

QuarkNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesdissociation01 natural sciencesDissociation (chemistry)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound stateInteracción entre cromoeléctico22 Física010306 general physicsconstituentpentaquarkPhysics010308 nuclear & particles physicschromoelectricstabilitymathematical methods: variationalEfectos cromomagnéticoslcsh:QC1-999Pentaquarkanti-charmConfiguraciones pentaquark QHigh Energy Physics - Phenomenologychromomagnetic[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]lcsh:Physics
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Deep inelastic scattering on the quark-gluon plasma

2020

We provide an interpretation of the structure functions of a thermal medium such as the quark-gluon plasma in terms of the scattering of an incoming electron on the medium via the exchange of a spacelike photon. We then focus on the deep-inelastic scattering (DIS) regime, and formulate the corresponding moment sum rules obeyed by the structure functions. Accordingly, these moments are given by the thermal expectation value of twist-two operators, which is computable from first principles in lattice QCD for the first few moments. We also show how lattice QCD calculations can be used to probe how large the photon virtuality needs to be in order for the Bjorken scaling of structure functions t…

QuarkNuclear and High Energy PhysicsParticle physicsFOS: Physical scienceshep-latPartonLattice QCDExpectation value01 natural sciencesHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPerturbative QCDlcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyPerturbative QCDParticle Physics - Latticehep-phLattice QCDRest frameDeep inelastic scatteringHigh Energy Physics - PhenomenologyQuark–gluon plasmaQuark-Gluon Plasmalcsh:QC770-798High Energy Physics::Experiment
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Weak decays of heavy hadrons into dynamically generated resonances

2016

In this paper, we present a review of recent works on weak decay of heavy mesons and baryons with two mesons, or a meson and a baryon, interacting strongly in the final state. The aim is to learn about the interaction of hadrons and how some particular resonances are produced in the reactions. It is shown that these reactions have peculiar features and act as filters for some quantum numbers which allow to identify easily some resonances and learn about their nature. The combination of basic elements of the weak interaction with the framework of the chiral unitary approach allow for an interpretation of results of many reactions and add a novel information to different aspects of the hadron…

QuarkNuclear and High Energy PhysicsParticle physicsFinal state interactionNuclear TheoryMesonNuclear TheoryHadronBaryon weak decaysFOS: Physical sciencesGeneral Physics and AstronomyHadronsLambda01 natural sciencesHeavy mesonNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesMesons (Nuclear physics)Mesons (Física nuclear)Nuclear Experiment010306 general physicsWave functionWeak interactions (Nuclear physics)PhysicsMesonic and baryonic resonances010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInteraccions febles (Física nuclear)State (functional analysis)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentProduction (computer science)International Journal of Modern Physics E
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DETERMINATION OF ALPHA-S FROM THE SCALING VIOLATION IN THE FRAGMENTATION FUNCTIONS IN E+E- ANNIHILATION

1993

A determination of the hadronic fragmentation functions of the Z0 boson is presented from a study of the inclusive hadron production with the DELPHI detector at LEP. These fragmentation functions were compared with the ones at lower energies, thus covering data in a large kinematic range: 196 less-than-or-equal-to Q2 less-than-or-equal-to 8312 GeV2 and x (= p(h)/E(beam)) > 0.08. A large scaling violation was observed, which was used to extract the strong coupling constant in second order QCD: alpha(s)(M(Z)) = 0.118 +/- 0.005. The corresponding QCD scale for five quark flavours is: LAMBDA(MS)(5)BAR = 230 +/- 60 MeV.

QuarkNuclear and High Energy PhysicsParticle physicsHADRONIC-Z-DECAYS; JET PRODUCTION-RATES; LUND MONTE-CARLO; LEADING ORDER; QUANTUM CHROMODYNAMICS; PERTURBATIVE QCD; PARTON DENSITIES; RESONANCE; SCATTERING; PHYSICSLUND MONTE-CARLOHigh Energy Physics::LatticeElectron–positron annihilationHadronElementary particlePARTON DENSITIES01 natural sciencesNuclear physicsPHYSICS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PERTURBATIVE QCDSCATTERING010306 general physicsNuclear ExperimentBosonQuantum chromodynamicsPhysicsCoupling constantAnnihilationQUANTUM CHROMODYNAMICS010308 nuclear & particles physicsJET PRODUCTION-RATESLEADING ORDERHigh Energy Physics::PhenomenologyRESONANCEFísica nuclearHigh Energy Physics::ExperimentParticle Physics - ExperimentHADRONIC-Z-DECAYSPHYSICS LETTERS B
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Third family quark–lepton unification at the TeV scale

2018

We construct a model of quark-lepton unification at the TeV scale based on an $SU(4)$ gauge symmetry, while still having acceptable neutrino masses and enough suppression in flavor changing neutral currents. An approximate $U(2)$ flavor symmetry is an artifact of family-dependent gauge charges leading to a natural realization of the CKM mixing matrix. The model predicts sizeable violation of PMNS unitarity as well as a gauge vector leptoquark $U_1^\mu = ({\bf 3}, {\bf 1}, 2/3)$ which can be produced at the LHC -- both effects within the reach of future measurements. In addition, recently reported experimental anomalies in semi-leptonic $B$-meson decays, both in charged $b \to c \tau \nu$ an…

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesLeptoquark010306 general physicsGauge symmetryPhysicsUnitarity010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySymmetry (physics)lcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoAnomaly (physics)lcsh:PhysicsLeptonPhysics Letters B
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Light hadron spectrum, renormalization constants and light quark masses with two dynamical fermions

2004

The results of a preliminary partially quenched (N_f=2) study of the light hadron spectrum, renormalization constants and light quark masses are presented. Numerical simulations are carried out with the LL-SSOR preconditioned Hybrid Monte Carlo with two degenerate dynamical fermions, using the plaquette gauge action and the Wilson quark action at beta = 5.8. Finite volume effects have been investigated employing two lattice volumes: 16^3 x 48 and 24^3 x 48. Configurations have been generated at four values of the sea quark mass corresponding to M_{PS}/M_V ~ 0.6 - 0.8.

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHadronFOS: Physical sciences01 natural sciences7. Clean energyMass fermionsRenormalizationHybrid Monte CarloHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)0103 physical sciencesQuantum chromodynamics; Lattices; Mass fermions010306 general physicsPhysicsFinite volume method010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]Degenerate energy levelsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaFermionLatticesAtomic and Molecular Physics and OpticsHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quantum chromodynamics
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The internal structure of jets at colliders: light and heavy quark inclusive hadronic distributions

2010

In this paper, we report our results on charged hadron multiplicities of heavy quark initiated jets produced in high energy collisions. After implementing the so-called dead cone effect in QCD evolution equations, we find that the average multiplicity decreases significantly as compared to the massless case. Finally, we discuss on the transverse momentum distribution of light quark initiated jets and emphasize on the comparison between our predictions and CDF data.

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHadronmultiplicitiesStructure (category theory)General Physics and AstronomyFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesJets010306 general physicsNuclear ExperimentPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMultiplicity (mathematics)inclusive distributionsMassless particleHigh Energy Physics - PhenomenologyDistribution (mathematics)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Transverse momentumHigh Energy Physics::Experiment
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Dirac and Pauli form factors from lattice QCD

2011

We present a comprehensive analysis of the electromagnetic form factors of the nucleon from a lattice simulation with two flavors of dynamical O(a)-improved Wilson fermions. A key feature of our calculation is that we make use of an extensive ensemble of lattice gauge field configurations with four different lattice spacings, multiple volumes, and pion masses down to m_\pi ~ 180 MeV. We find that by employing Kelly-inspired parametrizations for the Q^2-dependence of the form factors, we are able to obtain stable fits over our complete ensemble. Dirac and Pauli radii and the anomalous magnetic moments of the nucleon are extracted and results at light quark masses provide evidence for chiral …

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeLattice field theoryNuclear TheoryFOS: Physical sciences7. Clean energy01 natural sciencessymbols.namesakePauli exclusion principleHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Quantum field theory010306 general physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)FermionLattice QCDJHigh Energy Physics - PhenomenologysymbolsNucleon
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Faddeev study of heavy baryon spectroscopy

2007

16 pages, 3 figures.-- PACS nrs.: 12.39.Jh, 12.39.Pn, 14.20.-c.-- ISI Article Identifier: 000246249100015.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0703257

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryConstituent quarkFOS: Physical sciencesPosition and momentum spaceBottom quarkHyperfine interactionsHigh Energy Physics - Phenomenology (hep-ph)ChromodynamicsSymmetry breakingCharm (quantum number)Nuclear ExperimentPhysicsCharmed baryonsNonrelativistic quark modelsHigh Energy Physics::PhenomenologyFísicaQuantum numberFlip-flop modelBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNucleon-nucleon interactionBaryon spectra
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