Search results for "gluon"

showing 10 items of 697 documents

Comparison of Fragmentation Functions for Jets Dominated by Light Quarks and Gluons from pp and Pb+Pb Collisions in ATLAS

2019

Charged-particle fragmentation functions for jets azimuthally balanced by a high-transverse-momentum, prompt, isolated photon are measured in 25  pb^{-1} of pp and 0.49  nb^{-1} of Pb+Pb collision data at 5.02 TeV per nucleon pair recorded with the ATLAS detector at the Large Hadron Collider. The measurements are compared to predictions of Monte Carlo generators and to measurements of inclusively selected jets. In pp collisions, a different jet fragmentation function in photon-tagged events from that in inclusive jet events arises from the difference in fragmentation between light quarks and gluons. The ratios of the fragmentation functions in Pb+Pb events to that in pp events are used to e…

PhysicsLarge Hadron ColliderPhotonAstrophysics::High Energy Astrophysical PhenomenaGeneral Physics and AstronomyParton01 natural sciencesCharged particleNuclear physicsFragmentation (mass spectrometry)0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonJet quenchingPhysical Review Letters
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Monte Carlo Simulation for Elastic Energy Loss of Hard Partons in a Hydrodynamical Background

2011

We have developed a Monte Carlo simulation describing the $2 \rightarrow 2$ scatterings of perturbatively produced, non-eikonally propagating high-energy partons with the quarks and gluons of the expanding QCD medium created in ultrarelativistic heavy ion collisions. The partonic scattering rates are computed in leading-order perturbative QCD (pQCD), while three different hydrodynamical scenarios are used to model the strongly interacting medium. We compare our results and tune the model with the neutral pion suppression observed in $\sqrt{s_{NN}}=200$ GeV Au+Au collisions at the BNL-RHIC. We find the incoherent nature of elastic energy loss incompatible with the measured angular dependence…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderScatteringMonte Carlo methodNuclear TheoryHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesPartonHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Quark–gluon plasmaHigh Energy Physics::ExperimentNuclear Experiment
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A quark model analysis of Orbital Angular Momentum

1999

Orbital Angular Momentum (OAM) twist-two parton distributions are studied. At the low energy, hadronic, scale we calculate them for the relativistic MIT bag model and for non-relativistic potential quark models. We reach the scale of the data by leading order evolution using the OPE and perturbative QCD. We confirm that the contribution of quarks and gluons OAM to the nucleon spin grows with $Q^2$, and it can be relevant at the experimental scale, even if it is negligible at the hadronic scale, irrespective of the model used. The sign and shape of the quark OAM distribution at high $Q^2$ may depend strongly on the relative size of the OAM and spin distributions at the hadronic scale. Sizeab…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeQuark modelHigh Energy Physics::PhenomenologyNuclear TheoryPerturbative QCDFOS: Physical sciencesFísicaPartonGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quark–gluon plasmaHigh Energy Physics::ExperimentNucleonNuclear ExperimentSpin-½
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Highly occupied gauge theories in 2 + 1 dimensions : a self-similar attractor

2019

Motivated by the boost-invariant Glasma state in the initial stages in heavy-ion collisions, we perform classical-statistical simulations of SU(2) gauge theory in 2+1 dimensional space-time both with and without a scalar field in the adjoint representation. We show that irrespective of the details of the initial condition, the far-from-equilibrium evolution of these highly occupied systems approaches a unique universal attractor at high momenta that is the same for the gauge and scalar sectors. We extract the scaling exponents and the form of the distribution function close to this non-thermal fixed point. We find that the dynamics are governed by an energy cascade to higher momenta with sc…

quark-gluon plasmaScalar (mathematics)Adjoint representationhep-latFOS: Physical scienceshiukkasfysiikka114 Physical sciences01 natural sciencesComputer Science::Digital Librariessymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Correlation functionfysikk0103 physical sciencesAttractorquantum chromodynamicsGauge theory010306 general physicsUNIVERSAL DYNAMICSParticle Physics - PhenomenologyMathematical physicsDebyePhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)finite temperature field theoryParticle Physics - Latticehep-ph115 Astronomy Space scienceHigh Energy Physics - PhenomenologyDistribution functionsymbolsScalar fieldrelativistic heavy-ion collisions
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Transverse energy from minijets in ultrarelativistic nuclear collisions: a next-to-leading order analysis

2000

We compute in next-to-leading order (NLO) perturbative QCD the amount of transverse energy produced into a rapidity region $\Delta Y$ of a nuclear collision from partons created in the few-GeV subcollisions. The NLO formulation assumes collinear factorization and is based on the subtraction method. We first study the results as a function of the minimum transverse momentum scale and define and determine the associated $K$-factors. The dependence of the NLO results on the scale choice and on the size of $\Delta Y$ is also studied. The calculations are performed for GRV94 and CTEQ5 sets of parton distributions. Also the effect of nuclear shadowing to the NLO results is investigated. The main …

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesParton01 natural sciencesNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesQuark–gluon plasmaRapidityHigh Energy Physics::Experiment010306 general physicsNuclear Experiment
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Analytical results forO(αs)radiative corrections toe+e−→tt¯↑up to a given gluon energy cut

2009

We determine the O({alpha}{sub s}) radiative corrections to polarized top quark pair production in e{sup +}e{sup -} annihilations with a specified gluon energy cut. We write down fully analytical results for the unpolarized and polarized O({alpha}{sub s}) cross sections e{sup +}e{sup -}{yields}tt(G) and e{sup +}e{sup -}{yields}tt{sup {up_arrow}}(G) including their polar orientation dependence relative to the beam direction. In the soft-gluon limit we recover the usual factorizing form known from the soft-gluon approximation. In the limit when the gluon energy cut takes its maximum value we recover the totally inclusive unpolarized and polarized cross sections calculated previously. We provi…

Orientation (vector space)PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkAnnihilationPair productionElectron–positron annihilationHigh Energy Physics::PhenomenologyRadiative transferEnergy (signal processing)GluonPhysical Review D
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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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Investigation of the splitting of quark and gluon jets

1998

The splitting processes in identified quark and gluon jets are investigated using longitudinal and transverse observables. The jets are selected from symmetric three-jet events measured in Z decays L with the {\sc Delphi} detector in 1991-1994. Gluon jets are identified using heavy quark anti-tagging. Scaling violations in identified gluon jets are observed for the first time. The scale energy dependence of the gluon fragmentation function is found to be about two times larger than for the corresponding quark jets, consistent with the QCD expectation $C_A/C_F$. The primary splitting of gluons and quarks into subjets agrees with fragmentation models and, for specific regions of the jet resol…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Electron–positron annihilationAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::LatticeNuclear Theory7. Clean energy01 natural sciencesPartícules (Física nuclear)Nuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsHADRONIZATIONEngineering (miscellaneous)ScalingQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyObservableQCDPhoton structure functionHadronizationGluonMODELAVERAGE MULTIPLICITIES; QCD; HADRONIZATION; FRAGMENTATION; MODELFísica nuclearHigh Energy Physics::ExperimentFRAGMENTATIONAVERAGE MULTIPLICITIESParticle Physics - Experiment
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Initial state anisotropies and their uncertainties in ultrarelativistic heavy-ion collisions from the Monte Carlo Glauber model

2011

In hydrodynamical modeling of heavy-ion collisions, the initial-state spatial anisotropies are translated into momentum anisotropies of the final-state particle distributions. Thus, understanding the origin of the initial-state anisotropies and their uncertainties is important before extracting specific QCD matter properties, such as viscosity, from the experimental data. In this work we review the wounded nucleon approach based on the Monte Carlo Glauber model, charting in particular the uncertainties arising from modeling of the nucleon-nucleon interactions between the colliding nucleon pairs and nucleon-nucleon correlations inside the colliding nuclei. We discuss the differences between …

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)Nuclear Theoryta114010308 nuclear & particles physicsMonte Carlo methodNuclear TheoryFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)MomentumNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesQuark–gluon plasma010306 general physicsNucleonAnisotropyNuclear ExperimentGlauberQCD matterPhysical review C
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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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