Search results for "GLUON"

showing 10 items of 697 documents

High energy resummation of jet observables

2017

In this paper we investigate the extension of high energy resummation at LLx accuracy to jet observables. In particular, we present the high energy resummed expression of the transverse momentum distribution of the outgoing parton in the general partonic process $g(q) + g(q) \to g(q) + X$. In order to reach this result, several new ideas are introduced and exploited. First we prove that LLx resummation is achieved by dressing with hard radiation an off-shell gluon initiated LO process even if its on-shell limit is vanishing or trivial. Then we present a gauge-invariant framework where these calculations can be performed by using the modern helicity techniques. Finally, we show a possible wa…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)Perturbative QCDPartonObservableJet (particle physics)01 natural sciencesHelicityGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Perturbative QCD0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::ExperimentResummationResummation010306 general physicsJournal of High Energy Physics
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Precision predictions for the tt¯ production cross section at hadron colliders

2011

Abstract We make use of recent results in effective theory and higher-order perturbative calculations to improve the theoretical predictions of the top-quark pair production cross section at hadron colliders. In particular, we supplement the fixed-order NLO calculation with higher-order corrections from soft gluon resummation at NNLL accuracy. Uncertainties due to power corrections to the soft limit are estimated by combining results from single-particle inclusive and pair invariant-mass kinematics. We present our predictions as functions of the top-quark mass in both the pole scheme and the M S ¯ scheme. We also discuss the merits of using threshold masses as an alternative, and calculate …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadron01 natural sciencesGluonNuclear physicsRenormalizationCross section (physics)Pair production0103 physical sciencesEffective field theoryHigh Energy Physics::ExperimentLimit (mathematics)Resummation010306 general physicsPhysics Letters B
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Heavy ion collision multiplicities and gluon distribution functions

2001

Atomic number ($A$) and energy ($\roots$) scaling exponents of multiplicity and transverse energy in heavy ion collisions are analytically derived in the perturbative QCD + saturation model. The exponents depend on the small-$x$ behaviour of gluon distribution functions at an $x$-dependent scale. The relation between initial state and final state saturation is also discussed.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesMultiplicity (mathematics)Collision01 natural sciencesGluonTransverse planeHigh Energy Physics - PhenomenologyDistribution functionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesAtomic number010306 general physicsNuclear ExperimentScaling
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New Schwinger-Dyson equations for non-Abelian gauge theories

2008

We show that the application of the pinch technique to the conventional Schwinger-Dyson equations for the gluon propagator, gluon-quark vertex, and three-gluon vertex, gives rise to new equations endowed with special properties. The new series coincides with the one obtained in the Feynman gauge of the background field method, thus capturing the extensive gauge cancellations implemented by the pinch technique at the level of individual Green's functions. Its building blocks are the fully dressed pinch technique Green's functions obeying Abelian all-order Ward identities instead of the Slavnov-Taylor identites satisfied by their conventional counterparts. As a result, and contrary to the sta…

PhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaPropagatorFOS: Physical sciencesGluonsymbols.namesakeFormalism (philosophy of mathematics)High Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)PinchsymbolsFeynman diagramGauge theoryAbelian groupMathematical physics
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On dynamical gluon mass generation

2007

The effective gluon propagator constructed with the pinch technique is governed by a Schwinger-Dyson equation with special structure and gauge properties, that can be deduced from the correspondence with the background field method. Most importantly the non-perturbative gluon self-energy is transverse order-by-order in the dressed loop expansion, and separately for gluonic and ghost contributions, a property which allows for a meanigfull truncation. A linearized version of the truncated Schwinger-Dyson equation is derived, using a vertex that satisfies the required Ward identity and contains massless poles. The resulting integral equation, subject to a properly regularized constraint, is so…

PhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeMass generationHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesPropagatorIntegral equationGluonVertex (geometry)Massless particleHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PinchMathematical physics
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Polarized parton distributions and light-front dynamics

1998

We present a consistent calculation of the structure functions within a light-front constituent quark model of the nucleon. Relativistic effects and the relevance of the covariance constraints are analyzed for both polarized and unpolarized parton distributions. Various models, which differ in their gluonic structure at the hadronic scale, are investigated. The results of the full covariant calculation are compared with those of a non-relativistic approximation to show the structure and magnitude of the differences.

PhysicsNuclear and High Energy PhysicsParticle physicsCovarianceStructure functionsScale (ratio)Light-frontHadronNuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesConstituent quarkPartonCovarianceGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quark modelCovariant transformationHigh Energy Physics::ExperimentNucleonRelativistic quantum chemistryNuclear Experiment
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Complete next-to-leading order gluino contributions to and

2011

Abstract We present the first complete order α s corrections to the Wilson coefficients (at the high scale) of the various versions of magnetic and chromomagnetic operators which are induced by a squark–gluino exchange. For this matching calculation, we work out the on-shell amplitudes b → s γ and b → s g , both in the full and in the effective theory up to order α s 2 . The most difficult part of the calculation is the evaluation of the two-loop diagrams in the full theory; these can be split into two classes: a) diagrams with one gluino and a virtual gluon; b) diagrams with two gluinos or with one gluino and a four-squark vertex. Accordingly, the Wilson coefficients can be split into a pa…

PhysicsNuclear and High Energy PhysicsParticle physicsGluino010308 nuclear & particles physicsBranching fractionHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyBlock (permutation group theory)01 natural sciencesVertex (geometry)GluonRenormalization0103 physical sciencesEffective field theoryOrder (group theory)High Energy Physics::Experiment010306 general physicsNuclear Physics B
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J/ψ dissociation cross sections in a relativistic quark model

2003

We calculate the amplitudes and the cross sections of the charm dissociation processes J/\psi \pi => D \bar D, D* \bar D, D \bar D*, D* \bar D* within a relativistic constituent quark model. We consistently account for the contributions coming from both the box and triangle diagrams that contribute to the dissociation processes. The cross section is dominated by the D* \bar D and D* \bar D* channels. When summing up the four channels we find a maximum total cross section of about 2.3 mb at sqrt(s) \approx 4.1 GeV. We compare our results to the results of other model calculations.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyQuark modelHigh Energy Physics::PhenomenologyConstituent quarkHigh Energy Physics::ExperimentHeavy IonsQuark-gluon PlasmaDissociation (chemistry)
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Gluon mass through ghost synergy

2011

In this work we compute, at the "one-loop-dressed" level, the nonperturbative contribution of the ghost loops to the self-energy of the gluon propagator, in the Landau gauge. This is accomplished within the PT-BFM formalism, which guarantees the gauge-invariance of the emerging answer. In particular, the contribution of the ghost-loops is automatically transverse, by virtue of the QED-like Ward identities satisfied in this framework. Using as nonperturbative input the available lattice data for the ghost dressing function, we show that the ghost contributions have a rather sizable effect on the overall shape of the gluon propagator, both for $d=3,4$. Then, by exploiting a recently introduce…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPropagatorGluonFormalism (philosophy of mathematics)High Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)Mathematical physics
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THE PARTON DISTRIBUTIONS IN NUCLEONS: A QUARK MODEL ANALYSIS

1995

We use a laboratory frame description based on quark model wave functions to study the parton distributions in the nucleon. The present approach incorporates two major improvements, namely, it has the correct support and the renormalization group evolution is carried out to next-to-leading order. We obtain initially the parton distributions arising from the Isgur-Karl wave function. The failure of the latter to reproduce, even approximately, the data motivates us to analyze different scenarios, i.e. additional high momentum components and nonvanishing gluon distributions at the initial scale. We conclude that in order to understand data at various scales complex models simultaneously, it i…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyQuark modelGeneral Physics and AstronomyAstronomy and AstrophysicsPartonRenormalization groupWave functionNucleonHigh momentumGluonModern Physics Letters A
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