Search results for "quantum chromodynamics"

showing 10 items of 1027 documents

First Look at Two-Loop Five-Gluon Scattering in QCD.

2018

We compute the leading colour contributions to five-gluon scattering at two loops in massless QCD. The integrands of all independent helicity amplitudes are evaluated using d-dimensional generalised unitarity cuts and finite field reconstruction techniques. Numerical evaluation of the integral basis is performed with sector decomposition methods to obtain the first benchmark results for all helicity configurations of a 2 to 3 scattering process in QCD.

Quantum chromodynamicsPhysicsHigh Energy Physics - TheoryParticle physicsBasis (linear algebra)Unitarity010308 nuclear & particles physicsScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesHelicityGluonMassless particleDecomposition methods Finite fields Gluon scattering Helicities Scattering process UnitarityHigh Energy Physics - Phenomenology; High Energy Physics - Phenomenology; High Energy Physics - TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical sciencesPerturbation theory (quantum mechanics)010306 general physicsPhysical review letters
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Gluon mass and freezing of the QCD coupling

2007

Infrared finite solutions for the gluon propagator of pure QCD are obtained from the gauge-invariant non-linear Schwinger-Dyson equation formulated in the Feynman gauge of the background field method. These solutions may be fitted using a massive propagator, with the special characteristic that the effective mass employed drops asymptotically as the inverse square of the momentum transfer, in agreement with general operator-product expansion arguments. Due to the presence of the dynamical gluon mass the strong effective charge extracted from these solutions freezes at a finite value, giving rise to an infrared fixed point for QCD.

Quantum chromodynamicsPhysicsHistoryParticle physicsBackground field methodInfrared fixed pointHigh Energy Physics::LatticeMomentum transferHigh Energy Physics::PhenomenologyFísicaPropagatorFOS: Physical sciencesComputer Science ApplicationsEducationGluonsymbols.namesakeHigh Energy Physics - PhenomenologyEffective mass (solid-state physics)High Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicssymbolsFeynman diagram
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Cosmic implications of a low-scale solution to the axion domain wall problem

2019

The post-inflationary breaking of Peccei-Quinn (PQ) symmetry can lead to the cosmic domain wall catastrophe. In this Letter we show how to avoid domain walls implementing the Instanton Interference Effect (IIE) with a new interaction which itself breaks PQ symmetry and confines at an energy scale smaller than $\Lambda_{QCD}$. We give a general description of the mechanism and consider its cosmological implications and constraints within a minimal model. Contrary to other mechanisms we do not require an inverse phase transition neither fine-tuned bias terms. Incidentally, the mechanism leads to the introduction of new self-interacting dark matter candidates and the possibility of producing g…

Quantum chromodynamicsPhysicsInstantonParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesInverse01 natural sciencesHidden sectorDomain wall (string theory)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsAxionEnergy (signal processing)Astrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Results from pQCD for A+A collisions at RHIC & LHC energies

2000

This talk will discuss how to compute initial quantites in heavy ion collisions at RHIC (200 AGeV) and at LHC (5500 AGeV) using perturbative QCD (pQCD) by including the next-to-leading order (NLO) corrections and a dynamical determination of the dominant physical scale. The initial numbers are converted into final ones by assuming kinetic thermalization and adiabatic expansion.

Quantum chromodynamicsPhysicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesKinetic energyNuclear physicsHigh Energy Physics - PhenomenologyThermalisationHigh Energy Physics - Phenomenology (hep-ph)Heavy ionHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Adiabatic processNuclear Experiment
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Measurement of ϒ(1S) Elliptic Flow at Forward Rapidity in Pb-Pb Collisions at sNN=5.02  TeV

2019

The first measurement of the Υ(1S) elliptic flow coefficient (v2) is performed at forward rapidity (2.5 < y < 4) in Pb–Pb collisions at √sNN=5.02 TeV with the ALICE detector at the LHC. The results are obtained with the scalar product method and are reported as a function of transverse momentum (pT) up to 15 GeV/c in the 5%–60% centrality interval. The measured Υ(1S)v2 is consistent with 0 and with the small positive values predicted by transport models within uncertainties. The v2 coefficient in 2 < pT < 15 GeV/c is lower than that of inclusive J/ψ mesons in the same pT interval by 2.6 standard deviations. These results, combined with earlier suppression measurements, are in agreement with…

Quantum chromodynamicsPhysicsLarge Hadron ColliderMesonElliptic flowGeneral Physics and AstronomyQuarkonium01 natural sciencesStandard deviationNuclear physics0103 physical sciencesQuark–gluon plasmaRapidityNuclear Experiment010306 general physicsPhysical Review Letters
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Small-x physics at the LHeC

2018

The Large Hadron-electron Collider LHeC is a proposed upgrade of the LHC. It would add an electron beam to the LHC, and make it possible to study electron-proton and electron-nucleus collisions at very high energies. We present some of the highlights of the LHeC physics program related to the studies of partonic structure of protons and nuclei, and to the non-linear QCD phenomena visible at small $x$.

Quantum chromodynamicsPhysicsLarge Hadron ColliderNuclear TheoryNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical scienceshiukkasfysiikkalaw.inventionNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyUpgradeHigh Energy Physics - Phenomenology (hep-ph)lawPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)ColliderNuclear ExperimentydinfysiikkaNuclear theoryNuclear Experiment
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Production of π0 and η mesons in Cu+Au collisions at sNN=200GeV

2018

Production of π0 and η mesons has been measured at midrapidity in Cu+Au collisions at sNN=200GeV. Measurements were performed in π0(η)→γγ decay channel in the 1(2)-20GeV/c transverse momentum range. A strong suppression is observed for π0 and η meson production at high transverse momentum in central Cu+Au collisions relative to the p+p results scaled by the number of nucleon-nucleon collisions. In central collisions the suppression is similar to Au+Au with comparable nuclear overlap. The η/π0 ratio measured as a function of transverse momentum is consistent with mT-scaling parametrization down to pT=2GeV/c, its asymptotic value is constant and consistent with Au+Au and p+p and does not show…

Quantum chromodynamicsPhysicsMapleMeson productionMeson010308 nuclear & particles physicsNuclear Theorychemistry.chemical_elementengineering.material16. Peace & justice01 natural sciencesCopperNuclear physicsFragmentation (mass spectrometry)chemistry0103 physical sciencesQuark–gluon plasmaengineeringHigh Energy Physics::ExperimentImpact parameterNuclear Experiment010306 general physicsPhysical Review C
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Determination of resonance parameters in QCD by functional analysis methods

1988

A mathematically rigorous method based on functional analysis is used to determine resonance parameters of an amplitude from its given asymptotic expression in the space-like region. This method is checked on a model amplitude where both the asymptotic expression and the exact function are known. This method is then applied to the determination of the mass and the width of the ρ-meson from the corresponding space-like asymptotic QCD expression.

Quantum chromodynamicsPhysicsMathematical optimizationAmplitudePhysics and Astronomy (miscellaneous)Mathematical analysisElementary particleField theory (psychology)Function (mathematics)Quantum field theoryExpression (computer science)Engineering (miscellaneous)Resonance (particle physics)Zeitschrift für Physik C Particles and Fields
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Measurements of the Mass and Width of theηcMeson and of anηc(2S)Candidate

2004

The mass m(eta(c)) and total width Gamma(eta(c))(tot) of the eta(c) meson have been measured in two-photon interactions at the SLAC e(+)e(-) asymmetric B Factory with the BABAR detector. With a sample of approximately 2500 reconstructed eta(c)-->K(0)(S)K+/-pi(-/+) decays in 88 fb(-1) of data, the results are m(eta(c))=2982.5+/-1.1(stat)+/-0.9(syst) MeV/c(2) and Gamma(eta(c))(tot)=34.3+/-2.3(stat)+/-0.9(syst) MeV/c(2). Using the same decay mode, a second resonance with 112+/-24 events is observed with a mass of 3630.8+/-3.4(stat)+/-1.0(syst) MeV/c(2) and width of 17.0+/-8.3(stat)+/-2.5(syst) MeV/c(2). This observation is consistent with expectations for the eta(c)(2S) state.

Quantum chromodynamicsPhysicsMeson010308 nuclear & particles physicsAnalytical chemistryGeneral Physics and AstronomyResonance01 natural sciencesB-factoryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review Letters
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Topological susceptibility and η′ meson mass from Nf=2 lattice QCD at the physical point

2019

In this paper we explore the computation of topological susceptibility and ${\ensuremath{\eta}}^{\ensuremath{'}}$ meson mass in ${N}_{f}=2$ flavor QCD using lattice techniques with a physical value of the pion mass as well as larger pion mass values. We observe that the physical point can be reached without a significant increase in the statistical noise. The mass of the ${\ensuremath{\eta}}^{\ensuremath{'}}$ meson can be obtained from both fermionic two point functions and topological charge density correlation functions, giving compatible results. With the pion mass dependence of the ${\ensuremath{\eta}}^{\ensuremath{'}}$ mass being flat we arrive at ${M}_{{\ensuremath{\eta}}^{\ensuremath…

Quantum chromodynamicsPhysicsMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeLattice field theoryCharge densityLattice QCDTopology01 natural sciencesPionLattice (order)0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsTopological quantum numberPhysical Review D
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