Search results for "DGLAP"

showing 10 items of 26 documents

Nuclear parton distributions in the DGLAP approach

2001

Determination of the nuclear parton distributions within the framework of perturbative QCD, the DGLAP equations in particular, is discussed. Scale and flavour dependent nuclear effects in the parton distributions are compared with the scale and flavour independent parametrizations of HIJING and of the Hard Probe Collaboration. A comparison with the data from deep inelastic lepton-nucleus scattering and the Drell-Yan process in proton-nucleus collisions is shown.

PhysicsNuclear and High Energy PhysicsParticle physicsScale (ratio)ScatteringHigh Energy Physics::LatticeFlavourNuclear TheoryHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyPerturbative QCDFOS: Physical sciencesPartonHigh Energy Physics - PhenomenologyDGLAPHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNuclear ExperimentParticle Physics - Phenomenology
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Constraints for nuclear gluon shadowing from DIS data

2002

The $Q^2$ dependence of the ratios of the cross sections of deep inelastic lepton--nucleus scattering is studied in the framework of leading twist, lowest order perturbative QCD. The $\log Q^2$ slope of the ratio $F_2^{\rm Sn}/F_2^{\rm C}$ is computed by using the DGLAP evolution equations, and shown to be sensitive to the nuclear gluon distribution functions. Four different parametrizations for the nuclear effects of parton distributions are studied. We show that the NMC data on the $Q^2$ dependence of $F_2^{\rm Sn}/F_2^{\rm C}$ rule out the case where nuclear shadowing (suppression) of gluons at $x\sim 0.01$ is much larger than the shadowing observed in the ratio $F_2^A/F_2^{\rm D}$. We a…

PhysicsNuclear and High Energy PhysicsParticle physicsScatteringNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesPerturbative QCDOrder (ring theory)PartonGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)DGLAPDistribution functionHigh Energy Physics::ExperimentTwistNuclear ExperimentParticle Physics - PhenomenologyPhysics Letters B
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Global analysis of nuclear PDFs – latest developments

2013

Abstract In this review talk I discuss the latest developments in the DGLAP-based global analysis of nuclear parton distribution functions (nPDFs), focusing on the recent EPS09, nCTEQ and DSSZ global fits. I also briefly review the recent analysis for assigning a spatial dependence to the globally analysed nPDFs, resulting in the new sets EPS09s and EKS98s (“s” for spatial). With these, one can now compute nuclear hard-process cross sections and estimate their nPDF-originating uncertainties in different centrality classes for the first time consistently with the global nPDF fits.

PhysicsNuclear and High Energy PhysicsParticle physicsta114010308 nuclear & particles physicsParton01 natural sciencesDistribution functionDGLAP0103 physical sciencesSpatial dependence010306 general physicsCentralityNuclear theoryNuclear Physics A
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Constraints for nuclear PDFs from the LHCb D-meson data

2019

We quantify the impact of LHCb D-meson measurements at $\sqrt{s}=5 \, {\rm TeV}$ on the EPPS16 and nCTEQ15 nuclear PDFs. In our study, the theoretical description of D-meson production is based on the recently developed SACOT-$m_{\rm T}$ variant of the general-mass variable-flavour-number formalism, and the impact on PDFs is estimated via reweighting methods. We pay special attention on the theoretical uncertainties known to us, and are led to exclude the $p_{\rm T}<3 \, {\rm GeV}$ region from our main analysis. The LHCb data can be accommodated well within EPPS16 and nCTEQ15, and the data provide stringent constraints on the gluons in the shadowing/antishadowing regions. No evidence of …

PhysicsParticle physicsFormalism (philosophy)education05 social sciencesZero (complex analysis)FOS: Physical sciences020207 software engineeringhep-ph02 engineering and technologyhiukkasfysiikka114 Physical sciencesGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)DGLAPD meson0202 electrical engineering electronic engineering information engineering0501 psychology and cognitive sciencesProduction (computer science)ydinfysiikka050107 human factorsParticle Physics - Phenomenology
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The scale dependent nuclear effects in parton distributions for practical applications

1999

The scale dependence of the ratios of parton distributions in a proton of a nucleus $A$ and in the free proton, $R_i^A(x,Q^2)=f_{i/A}(x,Q^2)/f_i(x,Q^2)$, is studied within the framework of the lowest order leading-twist DGLAP evolution. By evolving the initial nuclear distributions obtained with the GRV-LO and CTEQ4L sets at a scale $Q_0^2$, we show that the ratios $R_i^A(x,Q^2)$ are only moderately sensitive to the choice of a specific modern set of free parton distributions. We propose that to a good first approximation, this parton distribution set-dependence of the nuclear ratios $R_i^A(x,Q^2)$ can be neglected in practical applications. With this result, we offer a numerical parametriz…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)ProtonNuclear TheoryFOS: Physical sciencesDrell–Yan processOrder (ring theory)Scale (descriptive set theory)PartonNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution (mathematics)DGLAPEngineering (miscellaneous)Parametrization
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Some remarks on dipole showers and the DGLAP equation

2009

It has been argued recently that parton showers based on colour dipoles conflict with collinear factorization and do not lead to the correct DGLAP equation. We show that this conclusion is based on an inappropriate assumption, namely the choice of the gluon energy as evolution variable. We further show numerically that Monte Carlo programs based on dipole showers with "infrared sensible" evolution variables reproduce the DGLAP equation both in asymptotic form as well as in comparison to the leading behaviour of second-order QCD matrix elements.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyMonte Carlo methodFOS: Physical sciencesPartonGluonDipoleColor modelHigh Energy Physics - PhenomenologyDGLAPHigh Energy Physics - Phenomenology (hep-ph)FactorizationHigh Energy Physics::Experiment
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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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A global reanalysis of nuclear parton distribution functions

2007

We determine the nuclear modifications of parton distribution functions of bound protons at scales $Q^2\ge 1.69$ GeV$^2$ and momentum fractions $10^{-5}\le x\le 1$ in a global analysis which utilizes nuclear hard process data, sum rules and leading-order DGLAP scale evolution. The main improvements over our earlier work {\em EKS98} are the automated $\chi^2$ minimization, simplified and better controllable fit functions, and most importantly, the possibility for error estimates. The resulting 16-parameter fit to the N=514 datapoints is good, $\chi^2/{\rm d.o.f}=0.82$. Within the error estimates obtained, the old {\em EKS98} parametrization is found to be fully consistent with the present an…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHadronFOS: Physical sciencesPartonGluonHigh Energy Physics - PhenomenologyDistribution functionDGLAPHigh Energy Physics - Phenomenology (hep-ph)Production (computer science)High Energy Physics::ExperimentNuclear ExperimentParametrization
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GENERALIZED PARTON DISTRIBUTIONS AND COMPOSITE CONSTITUENT QUARKS

2003

An approach is proposed to calculate Generalized Parton Distributions (GPDs) in a Constituent Quark Model (CQM) scenario, considering the constituent quarks as complex systems. The GPDs are obtained from the wave functions of the non relativistic CQM of Isgur and Karl, convoluted with the GPDs of the constituent quarks themselves. The latter are modelled by using the structure functions of the constituent quark, the double distribution representation of GPDs, and a recently proposed phenomenological constituent quark form factor. The present approach permits to access a kinematical range corresponding to both the DGLAP and the ERBL regions, for small values of the momentum transfer and of t…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeMomentum transferHigh Energy Physics::PhenomenologyForm factor (quantum field theory)FOS: Physical sciencesConstituent quarkFísicaPartonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution (mathematics)DGLAPBibliographyHigh Energy Physics::ExperimentNuclear Experiment
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An improved global analysis of nuclear parton distribution functions including RHIC data

2008

We present an improved leading-order global DGLAP analysis of nuclear parton distribution functions (nPDFs), supplementing the traditionally used data from deep inelastic lepton-nucleus scattering and Drell-Yan dilepton production in proton-nucleus collisions, with inclusive high-$p_T$ hadron production data measured at RHIC in d+Au collisions. With the help of an extended definition of the $\chi^2$ function, we now can more efficiently exploit the constraints the different data sets offer, for gluon shadowing in particular, and account for the overall data normalization uncertainties during the automated $\chi^2$ minimization. The very good simultaneous fit to the nuclear hard process data…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryHadronFOS: Physical sciencesDrell–Yan processPartonDeep inelastic scattering01 natural sciencesGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)DGLAP0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsParametrizationJournal of High Energy Physics
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