Search results for "quantum chromodynamics"

showing 10 items of 1027 documents

Measurement of the dijet invariant mass cross section in pp¯ collisions at s=1.96 TeV

2010

The inclusive dijet production double differential cross section as a function of the dijet invariant mass and of the largest absolute rapidity (y_{max}) of the two jets with the largest transverse momentum in an event is measured in proton anti-proton collisions at sqrt{s} = 1.96$ TeV using 0.7 fb^{-1} of data collected with the D0 detector at the Fermilab Tevatron Collider. The measurement is performed in six rapidity regions up to |y|=2.4. Next-to-leading order perturbative QCD predictions are found to be in agreement with the data.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronPerturbative QCD01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentInvariant massRapidityFermilabNuclear Experiment010306 general physicsColliderPhysics Letters B
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Measurement of theγγ*→π0transition form factor

2009

We study the reaction e+e- --> e+e-pi0 and measure the gamma gamma* --> pi0 transition form factor in the momentum transfer range from 4 to 40 GeV^2. The analysis is based on 442 fb^-1 of integrated luminosity collected at PEP-II with the BABAR detector at e+e- center-of-mass energies near 10.6 GeV.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsRange (particle radiation)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDetectorMomentum transferForm factor (quantum field theory)Dalitz plot01 natural sciences7. Clean energyMeasure (mathematics)LuminosityNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review D
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Transverse momenta of partons and dimuons in QCD

1978

Abstract Intrinsic (primordial) transverse momenta of quarks and gluons are calculated as well as those arising from recoil (bremsstrahlung) effects, using only the well-known parton distributions as input. The intrinsic kT's lie typically in the range of 150–250 MeV. Recent approaches using heuristic integro-differential equations for kT distributions of partons are shown to disagree with the results obtained by rigorous QCD calculations. The transverse momenta of dimuon pairs produced in pp → μ+μ− + X at the ISR can be solely explained by dynamical recoil effects, i.e., q q →(μ + μ − ) g and gq →(μ + μ − ) q , and no significant intrinsic transverse parton momenta are required. These dimu…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsRange (particle radiation)Large Hadron ColliderNuclear TheoryBremsstrahlungPartonNuclear physicsTransverse planeRecoilQuark–gluon plasmaHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics B
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ELFE: An electron laboratory for europe

2000

Abstract After about 10 years of discussions the physics case for ELFE, the Electron Laboratory For Europe, has become much clearer. The paper gives a personal view of the salient physics visible today. It is argued that QCD cannot be taken as the the “theory of strong interactions” as long as it cannot describe the hadronic world at low energies. New theoretical tools as “semi-exclusive reactions” and “off-forward-parton distributions” are promising new insight into hadrons by means of new observables. It is shown how connection of the new observables to QCD can be made. The most important parameters for an ELFE following from these conjectures are given allowing an experimental study of t…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsSalientHadronObservableElectronConnection (mathematics)Nuclear Physics A
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Scale evolution of nuclear parton distributions

1998

Using the NMC and E665 nuclear structure function ratios $F_2^A/F_2^D$ and $F_2^A/F_2^{C}$ from deep inelastic lepton-nucleus collisions, and the E772 Drell--Yan dilepton cross sections from proton-nucleus collisions, and incorporating baryon number and momentum sum rules, we determine nuclear parton distributions at an initial scale $Q_0^2$. With these distributions, we study QCD scale evolution of nuclear parton densities. The emphasis is on small values of $x$, especially on scale dependence of nuclear shadowing. As the main result, we show that a consistent picture can be obtained within the leading twist DGLAP evolution, and in particular, that the calculated $Q^2$ dependence of $F_2^{…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsScale (ratio)Nuclear TheoryNuclear TheoryHigh Energy Physics::PhenomenologyNuclear structureFOS: Physical sciencesPartonMomentumNuclear Theory (nucl-th)High Energy Physics - PhenomenologyDGLAPHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentBaryon numberTwistNuclear ExperimentParticle Physics - Phenomenology
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Description of the spacelike and timelike proton form factors at large momentum transfer in the QCD factorization approach

2012

Abstract We propose QCD factorization approach for description of the soft spectator scattering contribution. It is expected that such contribution is very important for description of the many exclusive processes at moderate values of Q 2 . Assuming the dominance of this mechanism we provide qualitative consideration of the proton form factors in the spacelike and timelike regions. Using the same approach we also provide estimates of the cross sections for the processes γ γ → p p and p p → γ γ at large energy and momentum transfer.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsTransfer (group theory)ProtonFactorizationScatteringMomentum transferEnergy–momentum relationProgress in Particle and Nuclear Physics
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Parton shower evolution in a 3-d hydrodynamical medium

2008

We present a Monte Carlo simulation of the perturbative Quantum Chromodynamics (pQCD) shower developing after a hard process embedded in a heavy-ion collision. The main assumption is that the cascade of branching partons traverses a medium which (consistent with standard radiative energy loss pictures) is characterized by a local transport coefficient qhat which measures the virtuality per unit length transferred to a parton which propagates in this medium. This increase in parton virtuality alters the development of the shower and in essence leads to extra induced radiation and hence a softening of the momentum distribution in the shower. After hadronization, this leads to the concept of a…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsTransport coefficientHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservablePartonHadronizationNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPerturbation theory (quantum mechanics)Parton showerNuclear Experiment
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The hadronic off-shell width of meson resonances

2000

6 páginas, 4 figuras.-- PACS number(s): 12.39.Fe, 12.38.Aw, 12.38.Cy, 12.40.Vv

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsUnitarityMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryForm factor (quantum field theory)PropagatorFísicaFOS: Physical sciencesVector meson dominanceHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentResummationNuclear Experiment
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N3LOHiggs boson and Drell-Yan production at threshold: The one-loop two-emission contribution

2014

In this paper, we study phenomenologically interesting soft radiation distributions in massless QCD. Specifically, we consider the emission of two soft partons off of a pair of lightlike Wilson lines, in either the fundamental or the adjoint representation, at next-to-leading order. Our results are an essential component of the next-to-next-to-next-to-leading order threshold corrections to both Higgs boson production in the gluon fusion channel and Drell-Yan lepton production. Our calculations are consistent with the recently published results for Higgs boson production. As a nontrivial cross-check on our analysis, we rederive a recent prediction for the Drell-Yan threshold cross section us…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsWilson loop010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDrell–Yan process01 natural sciencesGluonMassless particleDimensional regularization0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Renormalization group evolution of multi-gluon correlators in high energy QCD

2011

Many-body QCD in leading high energy Regge asymptotics is described by the Balitsky-JIMWLK hierarchy of renormalization group equations for the x evolution of multi-point Wilson line correlators. These correlators are universal and ubiquitous in final states in deeply inelastic scattering and hadronic collisions. For instance, recently measured di-hadron correlations at forward rapidity in deuteron-gold collisions at the Relativistic Heavy Ion Collider (RHIC) are sensitive to four and six point correlators of Wilson lines in the small x color fields of the dense nuclear target. We evaluate these correlators numerically by solving the functional Langevin equation that describes the Balitsky-…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsta114010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesInelastic scatteringRenormalization group01 natural sciencesGluonColor-glass condensateLangevin equationRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsRelativistic Heavy Ion ColliderNuclear ExperimentPhysics Letters B
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