Search results for "Gluon"

showing 10 items of 697 documents

Three-jet production at LEP and the bottom quark mass

1994

We consider the possibility of extracting the bottom quark mass from LEP data. The inclusive decay rate for $\zbb +\cdots$ is obtained at order $\as$ by summing up the one-loop two-parton decay rate to the tree-level three-parton rate. We calculate the decay width of the $Z$-boson into two and three jets containing the $b$-quark including complete quark mass effects. In particular, we give analytic results for a slight modification of the JADE clustering algorithm. We also study the angular distribution with respect to the angle formed between the gluon and the quark jets, which has a strong dependence on the quark mass. The impact of higher order QCD corrections on these observables is bri…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaOrder (ring theory)FOS: Physical sciencesObservableJet (particle physics)Bottom quarkJADE (particle detector)GluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentParticle Physics - Phenomenology
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Effective models of two-flavor QCD: from small towards large $m_q$

2009

We study effective models of chiral fields and Polyakov loop expected to describe the dynamics responsible for the phase structure of two-flavor QCD. We consider the chiral sector described either using a linear sigma model or a Nambu-Jona-Lasinio model and study how these models, on the mean-field level when coupled with the Polyakov loop, behave as a function of increasing bare quark (or pion) mass. We find qualitatively similar behaviors for the cases of the linear sigma model and the Nambu-Jona-Lasinio model and, by comparing with existing lattice data, show that one cannot conclusively decide which of the two approximate symmetries drives the phase transitions at the physical point.

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsPhase transitionSigma model010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Mean field theoryLattice (order)0103 physical sciencesQuark–gluon plasma010306 general physics
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Strange quark mass from Finite Energy QCD sum rules to five loops

2007

The strange quark mass is determined from a new QCD Finite Energy Sum Rule (FESR) optimized to reduce considerably the systematic uncertainties arising from the hadronic resonance sector. As a result, the main uncertainty in this determination is due to the value of $\Lambda_{QCD}$. The correlator of axial-vector divergences is used in perturbative QCD to five-loop order, including quark and gluon condensate contributions, in the framework of both Fixed Order (FOPT), and Contour Improved Perturbation Theory (CIPT). The latter exhibits very good convergence, leading to a remarkably stable result in the very wide range $s_0 = 1.0 - 4.0 {GeV}^2$, where $s_0$ is the radius of the integration co…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesStrange quarkHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Perturbative QCDFOS: Physical sciencesGluon condensateHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSum rule in quantum mechanicsNuclear Experiment
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Hadron structure at lowQ2

2007

This review deals with the structure of hadrons, strongly interacting many-body systems consisting of quarks and gluons. These systems have a size of about 1 fm, which shows up in scattering experiments at low momentum transfers $Q$ in the GeV region. At this scale the running coupling constant of Quantum Chromodynamics (QCD), the established theory of the strong interactions, becomes divergent. It is therefore highly intriguing to explore this theory in the realm of its strong interaction regime. However, the quarks and gluons can not be resolved at the GeV scale but have to be studied through their manifestations in the bound many-body systems, for instance pions, nucleons and their reson…

Quantum chromodynamicsQuarkPhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyStrong interactionFOS: Physical sciencesGeneral Physics and AstronomyLattice QCDHadronizationGluonNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quark–gluon plasmaHigh Energy Physics::ExperimentNuclear ExperimentReviews of Modern Physics
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On the temperature dependence of the electrical conductivity in hot quenched lattice QCD

2011

Extending our recent work, we report on a calculation of the vector current correlation function for light valence quarks in the deconfined phase of quenched QCD in the temperature range 1.16Tc<T<2.98Tc. After performing a systematic analysis of the in fluence of cut-off effects on light quark meson correlators using clover improved Wilson fermions, we discuss resulting constraints on the electrical conductivity in a quark gluon plasma.

Quantum chromodynamicsQuarkPhysicsfunctionNuclear and High Energy PhysicsValence (chemistry)MesonCondensed matter physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFermionLattice QCDQuark gluon plasmaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeElectrical resistivity and conductivityLight quark spectralQuark–gluon plasmaElectrical conductivityHigh Energy Physics::Experiment
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Identified charged particles in quark and gluon jets

2000

A sample of 2.2 million hadronic Z decays, selected from the data recorded by the Delphi detector at LEP during 1994-1995 was used for an improved measurement of inclusive distributions of pi+, K+ and p and their antiparticles in gluon and quark jets. The production spectra of the individual identified particles were found to be softer in gluon jets compared to quark jets, with a higher multiplicity in gluon jets as observed for inclusive charged particles. A significant proton enhancement in gluon jets is observed indicating that baryon production proceeds directly from colour objects. The maxima, xi^*, of the xi-distributions for kaons in gluon and quark jets are observed to be different.

QuarkAntiparticleParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHadronNuclear TheoryFOS: Physical sciences01 natural sciencesSpectral lineDECAYSPartícules (Física nuclear)High Energy Physics - ExperimentPHYSICSHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesALGORITHMMultiplicity (chemistry)010306 general physicsNuclear ExperimentEngineering (miscellaneous)DELPHIPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMULTIPLICITYORDER QCD; MULTIPLICITY; ALGORITHM; PHYSICS; DECAYSLARGE ELECTRON POSITRON COLLIDERCharged particleGluonBaryonPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentORDER QCDParticle Physics - Experiment
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Diffractive dijet production and Wigner distributions from the color glass condensate

2019

Experimental processes that are sensitive to parton Wigner distributions provide a powerful tool to advance our understanding of proton structure. In this work, we compute gluon Wigner and Husimi distributions of protons within the Color Glass Condensate framework, which includes a spatially dependent McLerran-Venugopalan initial configuration and the explicit numerical solution of the JIMWLK equations. We determine the leading anisotropy of the Wigner and Husimi distributions as a function of the angle between impact parameter and transverse momentum. We study experimental signatures of these angular correlations at a proposed Electron Ion Collider by computing coherent diffractive dijet p…

QuarkCOLLISIONSprotonitNuclear TheoryHIGH-ENERGY FACTORIZATIONFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciences114 Physical sciencesColor-glass condensateNuclear Theory (nucl-th)Nuclear physicsDEEP-INELASTIC SCATTERINGUNITARITYHigh Energy Physics - Phenomenology (hep-ph)Recoil0103 physical sciences010306 general physicsNuclear Experimentproton structureQuantum chromodynamicsPhysicsta114010308 nuclear & particles physicsQUARKNONLINEAR GLUON EVOLUTIONQCDGluonHigh Energy Physics - Phenomenologyparton Wigner distributionsEP SCATTERINGSATURATIONPHOTOPRODUCTIONcolor glass condensateImpact parameterNucleonPhysical Review D
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Imaging the nucleus with high-energy photons

2019

In the 1930's, nuclear physicists developed the first realistic atomic models, showing that nuclei were made up of protons and neutrons. In the 1960's, Deep Inelastic Scattering experiments showed that protons and neutrons had internal structure: quarks and gluons (collectively, partons), and later experiments showed that the parton momentum distributions are different in heavy nuclei, compared to those in free nucleons. This difference is not surprising; partons are sensitive to their environment, and two gluons from different nucleons may fuse together, for example. Understanding how quarks and gluons behave in the nuclear environment is a significant focus of modern nuclear physics. Rece…

QuarkNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesParton01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear structureGluonHigh Energy Physics - PhenomenologyQuark–gluon plasmaHigh Energy Physics::ExperimentNucleon
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Heavy quark momentum diffusion coefficient in 3D gluon plasma

2020

We study the heavy-quark momentum diffusion coefficient in far from equilibrium gluon plasma in a self-similar regime using real-time lattice techniques. We use 3 methods for the extraction: an unequal time electric field 2-point correlator integrated over the time difference, a spectral reconstruction (SR) method based on the measured equal time electric field correlator and a kinetic theory (KT) formula. The time-evolution of the momentum diffusion coefficient extracted using all methods is consistent with an approximate $t^{\frac{-1}{2}}$ power law. We also study the extracted diffusion coefficient as a function of the upper limit of the time integration and observe that including the in…

QuarkNuclear and High Energy PhysicsInfraredInitial stagesTransporthep-latFOS: Physical sciencesGlasmaHeavy flavour01 natural sciencesPower law114 Physical sciencesMomentum diffusionDiffusionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Electric fieldLattice (order)0103 physical sciencesPre-equilibrium dynamics010306 general physicsParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Particle Physics - Latticehep-phPlasmaGluonHigh Energy Physics - PhenomenologyQuantum electrodynamicsNuclear Physics A
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Heavy quark diffusion in an overoccupied gluon plasma

2020

We extract the heavy-quark diffusion coefficient \kappa and the resulting momentum broadening in a far-from-equilibrium non-Abelian plasma. We find several features in the time dependence of the momentum broadening: a short initial rapid growth of , followed by linear growth with time due to Langevin-type dynamics and damped oscillations around this growth at the plasmon frequency. We show that these novel oscillations are not easily explained using perturbative techniques but result from an excess of gluons at low momenta. These oscillation are therefore a gauge invariant confirmation of the infrared enhancement we had previously observed in gauge-fixed correlation functions. We argue that…

QuarkNuclear and High Energy PhysicsNuclear Theorynucl-thhep-latFOS: Physical sciencesLattice QCDhiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)fysikk0103 physical sciencesHeavy Quark Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsPlasmonParticle Physics - PhenomenologyPhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]010308 nuclear & particles physicsOscillationComputer Science::Information RetrievalHigh Energy Physics - Lattice (hep-lat)Particle Physics - Latticehep-phLattice QCDPlasmaInvariant (physics)GluonHigh Energy Physics - PhenomenologyQuantum electrodynamicsNuclear Physics - TheoryQuark–gluon plasmaQuark-Gluon Plasmalcsh:QC770-798
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