Search results for "Gluon"

showing 10 items of 697 documents

Centrality dependence of multiplicities in ultrarelativistic nuclear collisions

2000

We compute the centrality dependence of multiplicities of particles produced in ultrarelativistic nuclear collisions at various energies and atomic numbers. The computation is carried out in perturbative QCD with saturated densities of produced gluons and by including effects of nuclear geometry. Numbers are given for Au+Au collisions at RHIC energies.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsComputationNuclear TheoryFOS: Physical sciencesPerturbative QCD01 natural sciencesGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesAtomic number010306 general physicsCentralityNuclear Experiment
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Understanding saturation and AA collisions with an eA collider

2009

The initial conditions in high energy nucleus-nucleus collisions are determined by the small momentum fraction part of the nuclear wavefunction. This is the regime of gluon saturation and the most direct way to experimentally study it would be deep inelastic scattering at a high energy electron ion collider (EIC). This talk discusses some of the connections between physics at the EIC and the initial stage of relativistic heavy ion collisions. We argue that measurements at an EIC will provide detailed high-precision information about the parameters for the initial conditions, transverse geometry and longitudinal correlations that will be crucial in understanding the initial stage of a heavy …

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryFOS: Physical sciencesElectronDeep inelastic scatteringlaw.inventionGluonIonNuclear Theory (nucl-th)Nuclear physicsMomentumHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawColliderSaturation (chemistry)Wave functionNuclear Experiment
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EPS09 - a New Generation of NLO and LO Nuclear Parton Distribution Functions

2009

We present a next-to-leading order (NLO) global DGLAP analysis of nuclear parton distribution functions (nPDFs) and their uncertainties. Carrying out an NLO nPDF analysis for the first time with three different types of experimental input -- deep inelastic $\ell$+A scattering, Drell-Yan dilepton production in p+$A$ collisions, and inclusive pion production in d+Au and p+p collisions at RHIC -- we find that these data can well be described in a conventional collinear factorization framework. Although the pion production has not been traditionally included in the global analyses, we find that the shape of the nuclear modification factor $R_{\rm dAu}$ of the pion $p_T$-spectrum at midrapidity …

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesPartonGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyPionDGLAPDistribution functionHigh Energy Physics - Phenomenology (hep-ph)FactorizationHigh Energy Physics::ExperimentSensitivity (control systems)Nuclear ExperimentQCD matter
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Dilepton rapidity distributions from a hadronizing quark-gluon plasma

1995

Abstract We calculate the rapidity distribution of dilepton pairs produced from an evolving quark-gluon plasma assuming a longitudinal scaling expansion with initial conditions locally determined from the rapidity density. These distributions are compared with those from lowest-order Drell-Yan production and semileptonic charm decays.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyPlasmaNuclear physicsDistribution (mathematics)Quark–gluon plasmaHigh Energy Physics::ExperimentRapidityCharm (quantum number)Nuclear ExperimentScalingNuclear Physics A
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Screened potential and quarkonia properties at high temperatures

2009

We perform a quark model calculation of the quarkonia b (b) over bar and c (c) over bar spectra using smooth and sudden string breaking potentials. The screening parameter is scale dependent and can be related to an effective running gluon mass that has a finite infrared fixed point. A temperature dependence for the screening mass is motivated by lattice QCD simulations at finite temperature. Qualitatively different results are obtained for quarkonia properties close to a critical value of the deconfining temperature when a smooth or a sudden string breaking potential is used. In particular, with a sudden string breaking potential quarkonia radii remain almost independent of the temperature…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryInfrared fixed pointScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyQuark modelFísicaFOS: Physical sciencesLattice QCDCritical valueGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Critical point (thermodynamics)Nuclear ExperimentPhenomenology (particle physics)The European Physical Journal A
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Centrality categorization forRp(d)+Ain high-energy collisions

2014

High-energy proton- and deuteron-nucleus collisions provide an excellent tool for studying a wide array of physics effects, including modifications of parton distribution functions in nuclei, gluon saturation, and color neutralization and hadronization in a nuclear environment, among others. All of these effects are expected to have a significant dependence on the size of the nuclear target and the impact parameter of the collision, also known as the collision centrality. In this article, we detail a method for determining centrality classes in p(d) + A collisions via cuts on the multiplicity at backward rapidity (i.e., the nucleus-going direction) and for determining systematic uncertainti…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryMonte Carlo methodPartonGluonHadronizationNuclear physicsNeutronRapidityImpact parameterNuclear ExperimentRelativistic Heavy Ion ColliderPhysical Review C
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Small x physics and RHIC data

2010

This is a review of applications of the Color Glass Condensate to the phenomenology of relativistic heavy ion collisions. The initial stages of the collision can be understood in terms of the nonperturbatively strong nonlinear glasma color fields. We discuss how the CGC framework can and has been used to compute properties of the initial conditions of AA collisions. In particular this has led to recent progress in understanding multiparticle correlations, which can provide a directly observable signal of the properties of the initial stage of the collision process.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theoryta114010308 nuclear & particles physicsFOS: Physical sciencesGeneral Physics and AstronomyObservableCollisionDeep inelastic scattering01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesQuark–gluon plasmaBibliographyImpact parameterNuclear Experiment010306 general physicsPhenomenology (particle physics)Computer Science::DatabasesInternational Journal of Modern Physics E
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Search for the sgoldstino at √s = 189 to 202 GeV.

2000

A search for the supersymmetric partner of the goldstino, the sgoldstino S, at LEP2 is presented. The production Sgamma followed by S decay into two gluons or into two photons was studied at 189 - 202 GeV LEP centre-of-mass energies. No evidence for the S production was found and limits on the S mass corresponding to different theory parameters are given.

PhysicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physicsHigh Energy Physics::Phenomenology01 natural sciencesPartícules (Física nuclear)GluonSgoldstino0103 physical sciencesHigh Energy Physics::ExperimentFísica nuclearGoldstino010306 general physics
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Measurement of Higgs boson production in the diphoton decay channel inppcollisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector

2014

A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5 fb(-1) of proton-proton collisions data at root s = 7 TeV and 20.3 fb(-1) at root s = 8 TeV collected by the ATLAS detector at the Large Hadron Collider. The number of observed Higgs boson decays to diphotons divided by the corresponding Standard Model prediction, called the signal strength, is found to be mu = 1.17 +/- 0.27 at the value of the Higgs boson mass measured by ATLAS, m(H) = 125.4 GeV. The analysis is optimized to measure the signal strengths for individual Higgs boson production processes at this value of m(H). They are found to be mu(ggF) = 1.32…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology7. Clean energy01 natural sciencesStandard ModelVector bosonGluonNuclear physicsmedicine.anatomical_structure13. Climate actionAtlas (anatomy)0103 physical sciencesHiggs bosonmedicineHigh Energy Physics::ExperimentCenter of mass010306 general physicsPhysical Review D
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Nonlinear corrections to the DGLAP equations in view of the HERA data

2002

The effects of the first nonlinear corrections to the DGLAP evolution equations are studied by using the recent HERA data for the structure function $F_2(x,Q^2)$ of the free proton and the parton distributions from CTEQ5L and CTEQ6L as a baseline. By requiring a good fit to the H1 data, we determine initial parton distributions at $Q_0^2=1.4$ GeV$^2$ for the nonlinear scale evolution. We show that the nonlinear corrections improve the agreement with the $F_2(x,Q^2)$ data in the region of $x\sim 3\cdot 10^{-5}$ and $Q^2\sim 1.5$ GeV$^2$ without paying the price of obtaining a worse agreement at larger values of $x$ and $Q^2$. For the gluon distribution the nonlinear effects are found to play…

PhysicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsFOS: Physical sciencesPartonScale (descriptive set theory)HERA01 natural sciencesGluonHigh Energy Physics - PhenomenologyNonlinear systemHigh Energy Physics - Phenomenology (hep-ph)Distribution (mathematics)DGLAP0103 physical sciences010306 general physicsParticle Physics - Phenomenology
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