Search results for "quarks"

showing 10 items of 68 documents

Dynamical twisted mass fermions with light quarks

2007

We present results of dynamical simulations with 2 flavours of degenerate Wilson twisted mass quarks at maximal twist in the range of pseudo scalar masses from 300 to 550 MeV. The simulations are performed at one value of the lattice spacing a \lesssim 0.1 fm. In order to have O(a) improvement and aiming at small residual cutoff effects, the theory is tuned to maximal twist by requiring the vanishing of the untwisted quark mass. Precise results for the pseudo scalar decay constant and the pseudo scalar mass are confronted with chiral perturbation theory predictions and the low energy constants F, \bar{l}_3 and \bar{l}_4 are evaluated with small statistical errors.

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMONTE-CARLO ALGORITHMCHIRAL PERTURBATION-THEORY; MONTE-CARLO ALGORITHM; GROSS-NEVEU MODEL; YANG-MILLS THEORY; LATTICE QCD; PHASE-STRUCTURE; WILSON QUARKS; HMC ALGORITHM; GAUGE ACTIONS; 2 FLAVORSHigh Energy Physics::LatticeLattice field theoryScalar (mathematics)FOS: Physical sciences2 FLAVORSGAUGE ACTIONS01 natural sciences7. Clean energyCHIRAL PERTURBATION-THEORYLATTICE QCDHigh Energy Physics - LatticeGross–Neveu modelWILSON QUARKS0103 physical sciencesddc:530Twist010306 general physicsPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaGROSS-NEVEU MODELFermionLattice QCDSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciYANG-MILLS THEORYPHASE-STRUCTUREHMC ALGORITHM
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Light meson physics from maximally twisted mass lattice QCD

2009

40 pages, 5 figures, 8 tables, 3 appendix.-- PACS: 11.15.Ha; 12.38.Gc; 12.39.Fe

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMesonHigh Energy Physics::LatticeFOS: Physical sciencesLattice QCD7. Clean energy01 natural sciencessymbols.namesakeHigh Energy Physics - LatticeLattice constantChiral perturbation theoryLattice (order)0103 physical sciences010306 general physicsPhysics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLight mesonsMeson physicsFísicaFermionLattice QCDTwisted mass quarksQCDStrong interactions3. Good healthSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciLattice QCD; Strong interactions; Meson physics; Twisted mass quarkssymbolsLow energy constantsLagrangian
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Two-parton contribution to the heavy-quark forward–backward asymmetry in NNLO QCD

2006

Forward-backward asymmetries, $A_{FB}^Q$, are important observables for the determination of the neutral-current couplings of heavy quarks in inclusive heavy quark production, $e^+ e^- \to \gamma^*, Z^* \to Q +X$. In view of the measurement perspectives on $A_{FB}^Q$ at a future linear collider, precise predictions of $A_{FB}^Q$ are required for massive quarks. We compute the contribution of the $Q \bar Q$ final state to $A_{FB}^Q$ to order $\as^2$ in the QCD coupling. We provide general formulae, and we show that this contribution to $A_{FB}^Q$ is infrared-finite. We evaluate these two-parton contributions for $b$ and $c$ quarks on and near the $Z$ resonance, and for $t$ quarks above thres…

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::Latticemedia_common.quotation_subjectNuclear TheoryFOS: Physical sciencesParton01 natural sciencesAsymmetrylaw.inventionNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesPERTURBATIVE QCDNuclear Experiment010306 general physicsCollidermedia_commonCondensed Matter::Quantum GasesPhysicsQuantum chromodynamicsCouplingASYMMETRY IN NNLO QCD010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceObservableHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentHEAVY QUARKSRADIATIVE CORRECTIONSNuclear Physics B
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String breaking by light and strange quarks in QCD

2019

The energy spectrum of a system containing a static quark anti-quark pair is computed for a wide range of source separations using lattice QCD with $N_\mathrm{f}=2+1$ dynamical flavours. By employing a variational method with a basis including operators resembling both the gluon string and systems of two separated static mesons, the first three energy levels are determined up to and beyond the distance where it is energetically favourable for the vacuum to screen the static sources through light- or strange-quark pair creation, enabling both these screening phenomena to be observed. The separation dependence of the energy spectrum is reliably parameterised over this saturation region with a…

QuarkNuclear and High Energy PhysicsStrange quarkParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesLattice QCD01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHeavy quarks0103 physical sciences010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice QCDQuarkoniumString breakinglcsh:QC1-999GluonHigh Energy Physics - PhenomenologyPair productionHigh Energy Physics::Experimentlcsh:PhysicsPhysics Letters
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Decay constants of B-mesons from non-perturbative HQET with two light dynamical quarks

2014

We present a computation of B-meson decay constants from lattice QCD simulations within the framework of Heavy Quark Effective Theory for the b-quark. The next-to-leading order corrections in the HQET expansion are included non-perturbatively. Based on Nf=2 gauge field ensembles, covering three lattice spacings a (0.08-0.05)fm and pion masses down to 190MeV, a variational method for extracting hadronic matrix elements is used to keep systematic errors under control. In addition we perform a careful autocorrelation analysis in the extrapolation to the continuum and to the physical pion mass limits. Our final results read fB=186(13)MeV, fBs=224(14)MeV and fBs/fB=1.203(65). A comparison with o…

QuarkParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHadronLattice field theoryNuclear Theoryhep-latFOS: Physical sciencesLattice QCD01 natural sciencesNuclear physicsRenormalizationPionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesMeson decayB mesonddc:530010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsHeavy Quark Effective Theory010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologyhep-phLattice QCDHigh Energy Physics - PhenomenologyBottom quarks[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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Triquark correlations and pentaquarks in a QCD sum rule approach

2005

The role of quark correlations in the description of hadron dynamics in many domains of physics, from low energy dynamics to very hot(dense) systems, is being appreciated. Strong correlations of two quarks (diquark) have been widely investigated in this respect. Recently, we have proposed a dynamical scheme to describe the $\Theta^+$ pentaquark in which also three quark correlations (triquark) were instrumental in producing a low mass exotic state. We perform a study, within the QCD sum rule approach including OPE and direct instanton contributions, of triquark correlations and obtain two quasi-bound light $ud\bar{s}$ color quark clusters of 800 MeV and 930 MeV respectively.

QuarkParticle physicsNuclear and High Energy PhysicsNuclear TheoryHigh Energy Physics::LatticeHadronNuclear TheoryQuarksFOS: Physical sciencesHadronsHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)InstantonOperator product expansionQuantum chromodynamicsPhysicsHigh Energy Physics::PhenomenologyFísicaPentaquarkPentaquarkDiquarkHigh Energy Physics - PhenomenologyExotic baryonHigh Energy Physics::ExperimentSum rule in quantum mechanics
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Search for the exotic Θ+ resonance in the NOMAD experiment

2006

12 pages, 16 figures.-- PACS nrs.: 13.15.+g; 13.60.Le; 13.87.Fh; 14.40.Ev.-- ISI Article Identifier: 000243973100007.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ex/0612063.-- et al.

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Protonneutrino; nutrino oscillations; quarksElectromagnetic Calorimeter7. Clean energy01 natural sciencesParticle identificationHigh Energy Physics - ExperimentNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Muon neutrino010306 general physicsEngineering (miscellaneous)Charged currentPhysicsNeutral current010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaTransition Radiation DetectorPositive-strangenessBaryonPhotoproductionHigh Energy Physics::ExperimentNeutrinoParticle Physics - ExperimentCharged Current Interactions
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Search for the Associated Production of the Standard-Model Higgs Boson in the All-Hadronic Channel

2009

We report on a search for the standard-model Higgs boson in pp collisions at s=1.96 TeV using an integrated luminosity of 2.0 fb(-1). We look for production of the Higgs boson decaying to a pair of bottom quarks in association with a vector boson V (W or Z) decaying to quarks, resulting in a four-jet final state. Two of the jets are required to have secondary vertices consistent with B-hadron decays. We set the first 95% confidence level upper limit on the VH production cross section with V(-> qq/qq('))H(-> bb) decay for Higgs boson masses of 100-150 GeV/c(2) using data from run II at the Fermilab Tevatron. For m(H)=120 GeV/c(2), we exclude cross sections larger than 38 times the standard-m…

QuarkParticle physicsStandardsFinal stateFermilab TevatronHiggs bosonTevatronFOS: Physical sciencesGeneral Physics and AstronomyElementary particleddc:500.201 natural sciences114 Physical sciencesStandard ModelVector bosonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decayTellurium compounds0103 physical sciencesJetsB-hadron decaysHigh energy physics010306 general physicsBosonsBosonStandard-model Higgs bosonsPhysicsIntegrated luminosityHIGGS BOSONModel predictionCross section010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyConfidence levelsUpper limits3. Good healthVector bosonProduction cross sectionBottom quarksSecondary verticesHiggs bosonCDFHigh Energy Physics::Experiment
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Hall–Post inequalities: Review and application to molecules and tetraquarks

2019

A review is presented of the Hall–Post inequalities that give lower-bounds to the ground-state energy of quantum systems in terms of energies of smaller systems. New applications are given for systems experiencing both a static source and inner interactions, as well as for hydrogen-like molecules and for tetraquarks in some quark models. In the latter case, the Hall–Post inequalities constrain the possibility of deeply-bound exotic mesons below the threshold for dissociation into two quark–antiquark mesons. We also emphasize the usefulness of the Hall–Post bounds in terms of 3-body energies when some 2-body subsystems are ill defined or do not support any bound state.

QuarkParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryMesonenergy: ground stateHigh Energy Physics::LatticeFOS: Physical sciencesGeneral Physics and Astronomyquark antiquarkHall-Post inequalitiesdissociation01 natural sciencesDissociation (chemistry)Nuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Tetraquark0103 physical sciencesBound stateMoleculemoleculesPhysics - Atomic and Molecular Clusters010306 general physicsQuantumPhysicsquark modeltetraquarksHall–Post inequality010308 nuclear & particles physicsHigh Energy Physics::Phenomenologymeson: exoticMolecule[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]bound stateHigh Energy Physics - PhenomenologyQuantum Gases (cond-mat.quant-gas)few-body systems[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Atomic and Molecular Clusters (physics.atm-clus)Condensed Matter - Quantum GasesFew BodybaryonsAnnals of Physics
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Molecular and compact four-quark states

2009

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

QuarkPhysicsExoticsNuclear and High Energy PhysicsParticle physicsBar (music)High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstronomy and AstrophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Bound stateQuark-modelsTetraquarksHigh Energy Physics::ExperimentInstrumentationCharmonium
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