Search results for "GLUON"

showing 10 items of 697 documents

Search for four-top-quark production in the single-lepton and opposite-sign dilepton final states in pp collisions at s=13  TeV with the ATLAS detect…

2019

A search for four-top-quark production, tttt, is presented. It is based on proton-proton collision data with a center-of-mass energy s=13 TeV collected by the ATLAS detector at the Large Hadron Collider during the years 2015 and 2016, corresponding to an integrated luminosity of 36.1 fb-1. Data are analyzed in both the single-lepton and opposite-sign dilepton channels, characterized by the presence of one or two isolated electrons or muons with high-transverse momentum and multiple jets. A data-driven method is used to estimate the dominant background from top-quark pair production in association with jets. No significant excess above the Standard Model expectation is observed. The result i…

PhysicsTop quarkParticle physicsLarge Hadron ColliderMuon010308 nuclear & particles physicsHigh Energy Physics::Phenomenology01 natural sciencesGluonStandard ModelPair productionmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Measurement of the higher-order anisotropic flow coefficients for identified hadrons in Au + Au collisions atsNN=200GeV

2016

Measurements of the anisotropic flow coefficients v2{Ψ2},v3{Ψ3},v4{Ψ4}, and v4{Ψ2} for identified particles (π±,K±, and p+p) at midrapidity, obtained relative to the event planes Ψm at forward rapidities in Au + Au collisions at sNN=200GeV, are presented as a function of collision centrality and particle transverse momenta pT. The vn coefficients show characteristic patterns consistent with hydrodynamical expansion of the matter produced in the collisions. For each harmonic n, a modified valence quark-number Nq scaling [plotting vn{Ψm}/(Nq)n/2 versus transverse kinetic energies (KET)/Nq] is observed to yield a single curve for all the measured particle species for a broad range of KET. A si…

PhysicsValence (chemistry)010308 nuclear & particles physicsHadronKinetic energy01 natural sciencesSpectral lineTransverse plane0103 physical sciencesQuark–gluon plasmaAtomic physicsImpact parameterNuclear Experiment010306 general physicsAnisotropyPhysical Review C
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Confronting the impact parameter dependent JIMWLK evolution with HERA data

2018

The small-$x$ evolution of protons is determined from numerical solutions of the JIMWLK equations, starting from an initial condition at moderate $x$ for a finite size proton. The resulting dipole amplitude is used to calculate the total reduced cross section $\sigma_r$ and charm reduced cross section $\sigma_{rc}$, as well as diffractive vector meson production. We compare results to experimental data from HERA and discuss fundamental problems arising from the regime sensitive to non-perturbative physics. We emphasize that information on the gluonic content of the proton, gluon spatial distributions and correlations over wide ranges in $x$, which can in principle be constrained by our stud…

Physicsparton densitiesParticle physicsprotonitta114protons010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryHERAhiukkasfysiikka7. Clean energy01 natural sciencesGluonColor-glass condensateHigh Energy Physics - Phenomenology0103 physical sciencesContent (measure theory)Saturation (graph theory)High Energy Physics::ExperimentProduction (computer science)Vector mesonImpact parameter010306 general physicsNuclear ExperimentPhysical Review D
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Solving the heat-flow problem with transient relativistic fluid dynamics

2014

Israel-Stewart theory is a causal, stable formulation of relativistic dissipative fluid dynamics. This theory has been shown to give a decent description of the dynamical behavior of a relativistic fluid in cases where shear stress becomes important. In principle, it should also be applicable to situations where heat flow becomes important. However, it has been shown that there are cases where Israel-Stewart theory cannot reproduce phenomena associated with heat flow. In this paper, we derive a relativistic dissipative fluid-dynamical theory from kinetic theory which provides a good description of all dissipative phenomena, including heat flow. We explicitly demonstrate this by comparing th…

Physics::Fluid DynamicsPhysicsNuclear and High Energy Physicsta114Quark–gluon plasmaDynamics (mechanics)Fluid dynamicsKinetic theory of gasesDissipative systemShear stressMechanicsTransient (oscillation)Boltzmann equationPhysical Review D
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Use of a running coupling in the NLO calculation of forward hadron production

2018

We address and solve a puzzle raised by a recent calculation [1] of the cross-section for particle production in proton-nucleus collisions to next-to-leading order: the numerical results show an un- reasonably large dependence upon the choice of a prescription for the QCD running coupling, which spoils the predictive power of the calculation. Specifically, the results obtained with a prescription formulated in the transverse coordinate space differ by one to two orders of magnitude from those obtained with a prescription in momentum space. We show that this discrepancy is an artefact of the interplay between the asymptotic freedom of QCD and the Fourier transform from coordinate space to mo…

Position and momentum spaceQCD EVOLUTION01 natural sciencesAsymptotic freedomquantum chromodynamics: correctionhard scatteringHigh Energy Physics - Phenomenology (hep-ph)coupling constant: energy dependencestrong interaction: coupling constantEQUATIONkvanttifysiikkaComputingMilieux_MISCELLANEOUSPhysicsQuantum chromodynamicsQUARKhigher-order: 1nuclear physicssddc:12.39.StHigh Energy Physics - Phenomenology12.38.Bxsymbolsydinfysiikkahadron: forward productionFOS: Physical sciences114 Physical sciencesRENORMALIZATION-GROUP12.38.Cysymbols.namesakeCross section (physics)Theoretical physicsquantum chromodynamics0103 physical sciencessirontarelativistic heavy-ion collisionCoordinate spacenumerical calculations010306 general physicsp nucleus: scatteringcorrection: higher-orderCouplingta114010308 nuclear & particles physics25.75.-qCOLOR GLASS CONDENSATENONLINEAR GLUON EVOLUTIONRenormalization groupFourier transformasymptotic freedom[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physical Review D
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Measurement of upsilon production in 7 TeV pp collisions at ATLAS

2013

Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UAM

Prompt J/Psi ProductionUpsilon meson01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Polarization[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQCQuantum chromodynamicsPhysicsLarge Hadron ColliderHeavy QuarkoniumSettore FIS/01 - Fisica SperimentaleCharmonium ProductionATLASJ-PsiHelicityLarge Hadron ColliderHadronic CollisionsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCpp collisionsParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsMesonCiências Naturais::Ciências Físicas530 PhysicsGluons:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2upsilon production; pp collisions ; ATLAS; detector530Nuclear physics0103 physical sciencesddc:530RapidityHigh Energy Physics010306 general physicsScience & TechnologyATLAS detector010308 nuclear & particles physicsBranching fractionFísicaQCDGluonOctet Quarkonia ProductionHADRON-HADRON COLLISIONSRoot-S=7 TevExperimental High Energy PhysicsHigh Energy Physics::ExperimentHeavy quarkonia
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"Table 1" of "Identified particles in quark and gluon jets."

1997

Y events.

QUARK --> P XGLUON --> LAMBDA XStrange productionQUARK --> K+ XQUARK --> LAMBDABAR XQUARK --> K- XE+ E- --> QUARK QUARKBAR GLUONQUARK --> PBAR X91.2GLUON --> CHARGED-HADRON XJet ProductionInclusiveQUARK --> CHARGED-HADRON XGLUON --> K- XGLUON --> P XE+ E- --> 3JETGLUON --> KS XQUARK --> LAMBDA XE+ E- ScatteringExclusiveGLUON --> PBAR XGLUON --> K+ XMULT/MULTGLUON --> LAMBDABAR XQUARK --> KS X
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"Table 2" of "Identified particles in quark and gluon jets."

1997

Mercedes events.

QUARK --> P XStrange productionQUARK --> K+ XQUARK --> K- XE+ E- --> QUARK QUARKBAR GLUONQUARK --> PBAR X91.2GLUON --> CHARGED-HADRON XJet ProductionInclusiveQUARK --> CHARGED-HADRON XGLUON --> K- XGLUON --> P XE+ E- --> 3JETE+ E- ScatteringExclusiveGLUON --> PBAR XGLUON --> K+ XMULT/MULT
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"Table 7" of "Identified Charged Particles in Quark and Gluon Jets"

2003

Jet flavor tagging is used. (C=DUSCB), (C=DUSC), (C=UDS) mean quark-jet flavors. CONST(C=GLUON/JET) is the ratio gluon/jet for all charged particles. 'Mercedes' events, three-fold symmetric events, the angle between three jets is 120 +- 15 deg.

QUARKBAR --> P XQUARK --> P XAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyE+ E- --> QUARK QUARKBAR GLUONQUARK --> PBAR X91.2MULTInclusiveGLUON --> P XE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentGLUON --> PBAR XQUARKBAR --> PBAR XMULT/MULT
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"Table 3" of "Identified Charged Particles in Quark and Gluon Jets"

2003

Jet flavor tagging is used. (C=DUSCB), (C=DUSC), (C=UDS) mean quark-jet flavors. CONST(C=GLUON/JET) is the ratio gluon/jet for all charged particles. 'Y' events, mirror symmetric events, the angle between the most energetic jet and other two jets is 150 +- 15 deg.

QUARKBAR --> P XQUARK --> P XHigh Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryHigh Energy Physics::PhenomenologyE+ E- --> QUARK QUARKBAR GLUONQUARK --> PBAR X91.2MULTInclusiveGLUON --> P XE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentGLUON --> PBAR XQUARKBAR --> PBAR XMULT/MULT
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