Search results for "Gluon"

showing 10 items of 697 documents

The Nielsen identities for the two-point functions of QED and QCD

1994

We consider the Nielsen identities for the two-point functions of full QCD and QED in the class of Lorentz gauges. For pedagogical reasons the identities are first derived in QED to demonstrate the gauge independence of the photon self-energy, and of the electron mass shell. In QCD we derive the general identity and hence the identities for the quark, gluon and ghost propagators. The explicit contributions to the gluon and ghost identities are calculated to one-loop order, and then we show that the quark identity requires that in on-shell schemes the quark mass renormalisation must be gauge independent. Furthermore, we obtain formal solutions for the gluon self-energy and ghost propagator i…

High Energy Physics - TheoryQuarkPhotonPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeLorentz transformationNuclear TheoryFOS: Physical sciences01 natural sciencesHigh Energy Physics::Theorysymbols.namesakeIdentity (mathematics)0103 physical sciences010306 general physicsEngineering (miscellaneous)Mathematical physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPropagatorGauge (firearms)GluonHigh Energy Physics - Theory (hep-th)symbolsHigh Energy Physics::ExperimentZeitschrift für Physik C Particles and Fields
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SUSY Ward identities for multi-gluon helicity amplitudes with massive quarks

2006

We use supersymmetric Ward identities to relate multi-gluon helicity amplitudes involving a pair of massive quarks to amplitudes with massive scalars. This allows to use the recent results for scalar amplitudes with an arbitrary number of gluons obtained by on-shell recursion relations to obtain scattering amplitudes involving top quarks.

High Energy Physics - TheoryQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeScalar (mathematics)Nuclear TheoryHigh Energy Physics::PhenomenologyRecursion (computer science)FOS: Physical sciencesSupersymmetryHelicityGluonScattering amplitudeHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::Experiment
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Decomposition of one-loop QCD amplitudes into primitive amplitudes based on shuffle relations

2013

We present the decomposition of QCD partial amplitudes into primitive amplitudes at one-loop level and tree level for arbitrary numbers of quarks and gluons. Our method is based on shuffle relations. This method is purely combinatorial and does not require the inversion of a system of linear equations.

High Energy Physics - TheoryQuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesSystem of linear equationsGluonHigh Energy Physics - PhenomenologyS-matrix theoryAmplitudeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum mechanicsQuark–gluon plasmaHigh Energy Physics::ExperimentMathematical physics
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Color charge correlations in the proton at NLO: Beyond geometry based intuition

2021

Color charge correlators provide fundamental information about the proton structure. In this Letter, we evaluate numerically two-point color charge correlations in a proton on the light cone including the next-to-leading order corrections due to emission or exchange of a perturbative gluon. The non-perturbative valence quark structure of the proton is modelled in a way consistent with high-$x$ proton structure data. Our results show that the correlator exhibits startlingly non-trivial behavior at large momentum transfer or central impact parameters, and that the color charge correlation depends not only on the impact parameter but also on the relative transverse momentum of the two gluon pr…

High Energy Physics - TheoryQuarkprotonitCOLLISIONSNuclear and High Energy PhysicsProtonFLOWQC1-999FOS: Physical sciencesGeometry114 Physical sciences01 natural sciencesMomentumGLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesSCATTERINGFIELDNUCLEON010306 general physicscolor charge correlatorsPhysicsprotons010308 nuclear & particles physicsPhysicsQUARKMomentum transferHigh Energy Physics - PhenomenologyDipoleHigh Energy Physics - Theory (hep-th)Impact parameterNucleonColor chargePhysics Letters B
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Forward dijets in proton-nucleus collisions at next-to-leading order: the real corrections

2021

Using the CGC effective theory together with the hybrid factorisation, we study forward dijet production in proton-nucleus collisions beyond leading order. In this paper, we compute the "real" next-to-leading order (NLO) corrections, i.e. the radiative corrections associated with a three-parton final state, out of which only two are being measured. To that aim, we start by revisiting our previous results for the three-parton cross-section presented in our previous paper. After some reshuffling of terms, we deduce new expressions for these results, which not only look considerably simpler, but are also physically more transparent. We also correct several errors in this process. The real NLO …

High Energy Physics - Theorydijet: productionNuclear and High Energy PhysicsParticle physicsNuclear TheoryProton[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]splittingFOS: Physical sciencescollinearParton01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)DGLAP equationHigh Energy Physics - Phenomenology (hep-ph)FactorizationfactorizationNLO Computations0103 physical sciencesRadiative transferEffective field theoryradiative correctionlcsh:Nuclear and particle physics. Atomic energy. Radioactivitypartonheavy ion phenomenology010306 general physicsp nucleus: scatteringPhysicsNLO computationshybrid010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]higher-order: 1Heavy Ion PhenomenologyGluonHigh Energy Physics - PhenomenologyDGLAPHigh Energy Physics - Theory (hep-th)kinematics[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]color glass condensatelcsh:QC770-798
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Momentum anisotropy effects for quarkonium in a weakly coupled quark-gluon plasma below the melting temperature

2017

In the early stages of heavy-ion collisions, the hot QCD matter expands more longitudinally than transversely. This imbalance causes the system to become rapidly colder in the longitudinal direction and a local momentum anisotropy appears. In this paper, we study the heavy-quarkonium spectrum in the presence of a small plasma anisotropy. We work in the framework of pNRQCD at finite temperature. We inspect arrangements of non-relativistic and thermal scales complementary to those considered in the literature. In particular, we consider temperatures larger and Debye masses smaller than the binding energy, which is a temperature range relevant for presently running LHC experiments. In this set…

High Energy Physics - Theoryheavy ion: scatteringNuclear Theoryhiukkasfysiikka01 natural sciences7. Clean energy[ PHYS.HTHE ] Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics - Phenomenology (hep-ph)quarkonium: heavyquarkonium: mass spectrum[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)AnisotropyNuclear Experiment[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]quark gluon: plasmaQCD matterDebyeQuantum chromodynamicsPhysics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]quarkonium: momentumQuarkoniumHigh Energy Physics - PhenomenologyQuantum electrodynamicssymbolsquarkonium[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesanisotropy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]plasma: anisotropyNuclear Theory (nucl-th)Momentumsymbols.namesake0103 physical sciencesplasma: expansionparticle physicsquantum chromodynamics: perturbation theory010306 general physicsquantum chromodynamics: matterquantum chromodynamics: nonrelativisticta114effect: anisotropy010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPlasmamomentum: anisotropyquarkonium: dissociationHigh Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quark–gluon plasma[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physical Review D
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Transverse momentum dependence of D-meson production in Pb-Pb collisions at √sNN = 2.76 TeV

2016

The production of prompt charmed mesons D0 , D+ and D∗+, and their antiparticles, was measured with the ALICE detector in Pb-Pb collisions at the centre-of-mass energy per nucleon pair, √ sNN, of 2.76 TeV. The production yields for rapidity |y| < 0.5 are presented as a function of transverse momentum, pT, in the interval 1–36 GeV/c for the centrality class 0–10% and in the interval 1–16 GeV/c for the centrality class 30–50%. The nuclear modification factor RAA was computed using a proton-proton reference at √ s = 2.76 TeV, based on measurements at √ s = 7 TeV and on theoretical calculations. A maximum suppression by a factor of 5–6 with respect to binary-scaled pp yields is observed for the…

High Energy Physics::ExperimentNuclear Experimentcharm physicsheavy ion experimentsquark gluon plasma
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"Table 1" 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.

High Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryHigh Energy Physics::PhenomenologyE+ E- --&gt; QUARK QUARKBAR GLUONQUARK --&gt; PI- X91.2QUARK --&gt; PI+ XMULTQUARKBAR --&gt; PI- XInclusiveQUARKBAR --&gt; PI+ XE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentGLUON --&gt; PI+ XGLUON --&gt; PI- XMULT/MULT
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"Table 4" 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.

High Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryHigh Energy Physics::PhenomenologyE+ E- --&gt; QUARK QUARKBAR GLUONQUARKBAR --&gt; CHARGED X91.2MULTInclusiveGLUON --&gt; CHARGED XQUARK --&gt; CHARGED XE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentMULT/MULT
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Deep inelastic scattering off quark-gluon plasma and its photon emissivity

2021

The photon emissivity of quark-gluon plasma probes the interactions in the medium and differs qualitatively between a weakly coupled and a strongly coupled plasma in the soft-photon regime. The photon emissivity is given by the product of kinematic factors and a spectral function associated with the two-point correlator of the electromagnetic current at lightlike kinematics. A certain Euclidean correlator at imaginary spatial momentum can be calculated in lattice QCD and is given by an integral over the relevant spectral function at lightlike kinematics. I present a first exploratory lattice calculation of this correlator. Secondly, I show how Euclidean correlators at imaginary spatial mome…

High Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)hep-latFOS: Physical scienceshep-phParticle Physics - LatticeLattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Quark-Gluon PlasmaHigh Energy Physics::ExperimentParticle Physics - Phenomenology
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