Search results for "Gluon"

showing 10 items of 697 documents

Measurements of e+e− pairs from open heavy flavor in p+p and d+A collisions at sNN=200 GeV

2017

We report a measurement of e+e− pairs from semileptonic heavy-flavor decays in p+p collisions at sNN=200 GeV. The e+e− pair yield from bb¯ and cc¯ is separated by exploiting a double differential fit done simultaneously in dielectron invariant mass and pT. We used three different event generators, pythia, mc@nlo, and powheg, to simulate the e+e− spectra from cc¯ and bb¯ production. The data can be well described by all three generators within the detector acceptance. However, when using the generators to extrapolate to 4π, significant differences are observed for the total cross section. These difference are less pronounced for bb¯ than for cc¯. The same model dependence was observed in alr…

Quantum chromodynamicsPhysicsParticle physics010308 nuclear & particles physicsDrell–Yan processParton01 natural sciencesSpectral lineNuclear physics0103 physical sciencesQuark–gluon plasmaRapidityInvariant massPerturbation theory (quantum mechanics)010306 general physicsPhysical Review C
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5 QCD on the Lattice

2008

Since Wilson’s seminal papers of the mid-1970s, the lattice approach to Quantum Chromodynamics has become increasingly important for the study of the strong interaction at low energies, and has now turned into a mature and established technique. In spite of the fact that the lattice formulation of Quantum Field Theory has been applied to virtually all fundamental interactions, it is appropriate to discuss this topic in a chapter devoted to QCD, since by far the largest part of activity is focused on the strong interaction. Lattice QCD is, in fact, the only known method which allows ab initio investigations of hadronic properties, starting from the QCD Lagrangian formulated in terms of quark…

Quantum chromodynamicsPhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryQCD vacuumQuark–gluon plasmaHigh Energy Physics::ExperimentLattice QCDChiral symmetry breakingFundamental interaction
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Heavy-flavour production in the SACOT-mT scheme

2019

The hadroproduction of heavy-flavoured mesons has recently attracted a growing interest e.g. within the people involved in global analysis of proton and nuclear parton distribution functions, saturation physics, and physics of cosmic rays. In particular, the D- and B-meson measurements of LHCb at forward direction are sensitive to gluon dynamics at small $x$ and are one of the few perturbative small-$x$ probes before the next generation deep-inelastic-scattering experiments. In this talk, we will concentrate on the collinear-factorization approach to inclusive D-meson production and describe a novel implementation --- SACOT-$m_{\rm T}$ --- of the general-mass variable flavour number scheme …

Quantum chromodynamicsPhysicsParticle physicsDistribution functionMesonProtonHigh Energy Physics::PhenomenologySaturation (graph theory)High Energy Physics::ExperimentProduction (computer science)PartonhiukkasfysiikkaGluonProceedings of International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear Collisions — PoS(HardProbes2018)
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Solution to the Flavor Problem of Warped Extra-Dimension Models

2011

A minimal solution to the flavor problem of warped extra-dimension models, i.e. the excessive mixed-chirality contribution to CP violation in K-Kbar mixing arising from Kaluza-Klein (KK) gluon exchange, is proposed. Extending the strong-interaction gauge group in the bulk by an additional SU(3), and breaking this symmetry to QCD via boundary conditions, the constraints arising from the epsilon_K parameter are significantly relaxed. As a result, KK scales M_KK ~ 2 TeV are consistent with all flavor observables without significant fine-tuning. The model predicts the existence of an extended Higgs sector featuring massive color-octet scalars and a tower of KK pseudo-axial gluon resonances, who…

Quantum chromodynamicsPhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyObservableSymmetry (physics)Higgs sectorGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Gauge groupCP violationHigh Energy Physics::ExperimentBoundary value problemPhysical Review Letters
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Accelerating Ab Initio Nucleon Structure Calculations with All-Mode-Averaging on Gordon

2014

The composition of nucleons has long been known to be sub-atomic particles called quarks and gluons, which interact through the strong force and theoretically can be described by Quantum Chromodynamics (QCD). Lattice QCD (LQCD), in which the continuous space-time is translated into grid points on a four-dimensional lattice and ab initio Monte Carlo simulations are performed, is by far the only model-independent method to study QCD with controllable errors. We report the successful application of a novel algorithm, All-Mode-Averaging, in the LQCD calculations of nucleon internal structure on the Gordon supercomputer our award of roughly 6 million service units through XSEDE. The application …

Quantum chromodynamicsPhysicsParticle physicsHigh Energy Physics::LatticeQuantum electrodynamicsLattice (order)High Energy Physics::PhenomenologyQuark–gluon plasmaMonte Carlo methodStrong interactionAb initioLattice QCDNucleonProceedings of the 2014 Annual Conference on Extreme Science and Engineering Discovery Environment
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Effective gluon mass and infrared fixed point in QCD

2007

We report on a special type of solutions for the gluon propagator of pure QCD, obtained from the corresponding non-linear Schwinger-Dyson equation formulated in the Feynman gauge of the background field method. These solutions reach a finite value in the deep infrared and may be fitted using a massive propagator, with the crucial characteristic that the effective ``mass'' employed depends on the momentum transfer. Specifically, the gluon mass falls off as the inverse square of the momentum, as expected from the operator-product expansion. In addition, one may define a dimensionless quantity, which constitutes the generalization in a non-Abelian context of the universal QED effective charge.…

Quantum chromodynamicsPhysicsParticle physicsInfrared fixed pointBackground field methodHigh Energy Physics::LatticeMomentum transferHigh Energy Physics::PhenomenologyFOS: Physical sciencesPropagatorFísicaAsymptotic freedomGluonsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicssymbolsFeynman diagram
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Gluon Mass, Glueballs and Gluonic Mesons

2011

We review the phenomenological and theoretical evidences for dynamical gluon mass generation and the main features of the glueball spectrum in (pure gauge) Yang-Mills theories. The mixing between glueball and conventional $\bar q q$ states in $f_0$ scalar mesons is discussed. For pseudoscalar mesons, the inclusion of the glue field in an effective low energy theory is presented leading to a third isoscalar $\eta''$ partner of the $\eta$ and $\eta'$. Branching ratios for processes involving $\eta''$ are given and, when available, compatible with data for $\eta(1405)$.

Quantum chromodynamicsPhysicsParticle physicsMesonGlueballHigh Energy Physics::LatticeIsoscalarNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesPseudoscalar mesonGluonNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNuclear ExperimentScalar mesonGluon fieldProceedings of The many faces of QCD — PoS(FacesQCD)
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Exploratory studies for the position-space approach to hadronic light-by-light scattering in the muon g - 2

2017

The well-known discrepancy in the muon $g-2$ between experiment and theory demands further theory investigations in view of the upcoming new experiments. One of the leading uncertainties lies in the hadronic light-by-light scattering contribution (HLbL), that we address with our position-space approach. We focus on exploratory studies of the pion-pole contribution in a simple model and the fermion loop without gluon exchanges in the continuum and in infinite volume. These studies provide us with useful information for our planned computation of HLbL in the muon $g-2$ using full QCD.

Quantum chromodynamicsPhysicsParticle physicsMuon010308 nuclear & particles physicsScatteringPhysicsQC1-999Computer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)HadronFOS: Physical sciencesPosition and momentum spaceFermion01 natural sciencesLight scatteringGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsEPJ Web of Conferences
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QCD effective charges from lattice data

2010

We use recent lattice data on the gluon and ghost propagators, as well as the Kugo-Ojima function, in order to extract the non-perturbative behavior of two particular definitions of the QCD effective charge, one based on the pinch technique construction, and one obtained from the standard ghost-gluon vertex. The construction relies crucially on the definition of two dimensionful quantities, which are invariant under the renormalization group, and are built out of very particular combinations of the aforementioned Green's functions. The main non-perturbative feature of both effective charges, encoded in the infrared finiteness of the gluon propagator and ghost dressing function used in their…

Quantum chromodynamicsPhysicsParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesPropagatorFísicaInvariant (physics)Renormalization groupQCDEffective nuclear chargeVertex (geometry)GluonTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeNonperturbative EffectsLattice (order)
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Recent results from PHENIX on the evolution of hot QCD

2014

The Relativistic Heavy Ion Collider’s (RHIC) energy scan program explores the phase transition between the hadron gas and the quark gluon plasma phases by varying center-of-mass energies from √sNN = 7.7 to 200 GeV and using various system sizes. The nuclear modification factor of π0 and the azimuthal anisotropy of charged hadrons were measured in Au+Au collisions at c.m. energies √sNN = 39, 62.4 and 200 GeV. In addition, we present recent results of direct photon yield and anisotropy measurements in Au+Au collisions at c.m. energy √sNN = 200 GeV.

Quantum chromodynamicsPhysicsParticle physicsPhase transitionta114PhysicsQC1-999HadronNUCLEUS-NUCLEUS COLLISIONSHigh Energy Physics::PhenomenologyNuclear TheoryModification factorCOLLABORATION7. Clean energyPhoton yield114 Physical sciencesNuclear physicsQuark–gluon plasmaHigh Energy Physics::ExperimentRelativistic Heavy Ion ColliderAnisotropyNuclear ExperimentMATTEREPJ Web of Conferences
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