Search results for "DGLAP"

showing 10 items of 26 documents

Enhancement of charm quark production due to nonlinear corrections to the DGLAP equations

2004

We have studied how parton distributions based on the inclusion of nonlinear scale evolution and constraints from HERA data affect charm production in $pp$ collisions at center-of-mass energies of 5.5, 8.8 and 14 TeV. We find that, while the resulting enhancement can be substantial, it is very sensitive to the charm quark mass and the scale entering the parton densities and the strong coupling constant.

Coupling constantPhysicsQuarkNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesPartonHERA01 natural sciencesCharm quarkNuclear physicsNuclear Theory (nucl-th)Nonlinear systemHigh Energy Physics - PhenomenologyDGLAPHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentCharm (quantum number)010306 general physicsNuclear Experiment
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Impact of dijet and D-meson data from 5.02 TeV p+Pb collisions on nuclear PDFs

2020

We discuss the new constraints on gluon parton distribution function (PDF) in lead nucleus, derivable with the Hessian PDF reweighting method from the 5.02 TeV p+Pb measurements of dijet (CMS) and $D^0$-meson (LHCb) nuclear modification ratios. The impact is found to be significant, placing stringent constraints in the mid- and previously unconstrained small-$x$ regions. The CMS dijet data confirm the existence of gluon anti-shadowing and the onset of small-$x$ shadowing, as well as reduce the gluon PDF uncertainties in the larger-$x$ region. The gluon constraints from the LHCb $D^0$ data, reaching down to $x \sim 10^{-5}$ and derived in a NLO perturbative QCD approach, provide a remarkable…

Hessian matrixNuclear and High Energy PhysicsParticle physicsdijet productionNuclear TheoryFOS: Physical sciencesnuclear parton distribution functionPartonopen heavy flavour114 Physical sciences7. Clean energy01 natural sciencessymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesD meson010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPerturbative QCDGluonUniversality (dynamical systems)proton–nucleus collisionHigh Energy Physics - PhenomenologyDistribution functionDGLAPsymbolsHigh Energy Physics::Experiment
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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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Fragmentation in the ϕ3 theory and the LPHD hypothesis

2015

We present analytic solution of the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equation at leading order (LO) in the phi^3 theory in 6 space-time dimensions. If the phi^3 model was the theory of strong interactions, the obtained solution would describe the distribution of partons in a jet. We point out that the local parton-hadron duality (LPHD) conjecture does not work in this hypothetical situation. That is, treatment of hadronisation of shower partons is essential for the description of hadron distributions in jets stemming from proton-proton (pp) collisions at \sqrt{s} = 7 TeV and from electron-positron (e+e-) annihilations at various collision energies. We use a statistical mod…

Nuclear and High Energy PhysicsParticle physicsHadronFOS: Physical sciencesParton01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)Fragmentation (mass spectrometry)0103 physical sciencesNuclear Experiment010306 general physicsquantum field theoryPhysicsConjectureta114local parton-hadron duality010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsStatistical modelCollisionAtomic and Molecular Physics and OpticsHadronizationHigh Energy Physics - PhenomenologyDGLAPHigh Energy Physics::Experimentphi^3 theoryhadronizationInternational Journal of Modern Physics A
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Enhanced charm hadroproduction due to nonlinear corrections to the DGLAP equations

2004

We have studied the effects of nonlinear scale evolution of the parton distribution functions to charm production in $pp$ collisions at center-of-mass energies of 5.5, 8.8 and 14 TeV. We find that the differential charm cross section can be enhanced up to a factor of 4-5 at low $p_T$. The enhancement is quite sensitive to the charm quark mass and the renormalization/factorization scales.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesParton01 natural sciencesCharm quarkRenormalizationNonlinear systemHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)DGLAPDistribution functionFactorization0103 physical sciencesHigh Energy Physics::ExperimentCharm (quantum number)010306 general physicsNuclear Experiment
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Nuclear PDFs at NLO - status report and review of the EPS09 results

2011

We review the current status of the global DGLAP analysis of nuclear parton distribution functions, nPDFs, focusing on the recent EPS09 analysis, whose output, EPS09NLO, is the best-constrained NLO nPDF set on the market. Collinear factorization is found to work very well in the kinematical region studied. With the error sets released in the EPS09 package one can compute how the nPDF-related uncertainties propagate into factorizable nuclear hard-process cross sections. A comparison with the other existing NLO nPDF sets is shown, and the BRAHMS forward-$\eta$ hadron data from d+Au collisions are discussed in the light of the EPS09 nPDFs and their error sets.

PhysicsNuclear and High Energy PhysicsParticle physicsCurrent (mathematics)Nuclear Theoryta114010308 nuclear & particles physicsHadronPerturbative QCDFOS: Physical sciencesPartonStatus report01 natural sciencesNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyDGLAPDistribution functionHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciences010306 general physicsNuclear Physics A
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Nuclear Parton Distributions - a DGLAP Analysis

1999

Nuclear parton distributions $f_A(x,Q^2)$ are studied within a framework of the DGLAP evolution. Measurements of $F_2^A/F_2^D$ in deep inelastic $lA$ collisions, and Drell--Yan dilepton cross sections measured in $pA$ collisions are used as constraints. Also conservation of momentum and baryon number is required. It is shown that the calculated $Q^2$ evolution of $F_2^{\rm Sn}/F_2^{\rm C}$ agrees very well with the recent NMC data, and that the ratios $R_f^A=f_A/f$ are only moderately sensitive to the choice of a specific modern set of free parton distributions. For general use, we offer a numerical parametrization of $R_f^A(x,Q^2)$ for all parton flavours $f$ in $A>2$, and at $10^{-6}\l…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyDGLAPHigh Energy Physics - Phenomenology (hep-ph)FOS: Physical sciencesPartonBaryon numberParametrization
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DGLAP analyses of nPDF: constraints from data

2002

We explain how the constraints from present experimental data can be used to obtain the nPDF in the framework of LO DGLAP evolution. We will also compare the only two available sets of this type and comment on the important information that neutrino factories could provide.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)DGLAPFOS: Physical sciencesExperimental dataHigh Energy Physics::ExperimentNeutrinoParticle Physics - Phenomenology
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EPS09 - a New Generation of NLO and LO Nuclear Parton Distribution Functions

2009

We present a next-to-leading order (NLO) global DGLAP analysis of nuclear parton distribution functions (nPDFs) and their uncertainties. Carrying out an NLO nPDF analysis for the first time with three different types of experimental input -- deep inelastic $\ell$+A scattering, Drell-Yan dilepton production in p+$A$ collisions, and inclusive pion production in d+Au and p+p collisions at RHIC -- we find that these data can well be described in a conventional collinear factorization framework. Although the pion production has not been traditionally included in the global analyses, we find that the shape of the nuclear modification factor $R_{\rm dAu}$ of the pion $p_T$-spectrum at midrapidity …

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesPartonGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyPionDGLAPDistribution functionHigh Energy Physics - Phenomenology (hep-ph)FactorizationHigh Energy Physics::ExperimentSensitivity (control systems)Nuclear ExperimentQCD matter
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Nonlinear corrections to the DGLAP equations in view of the HERA data

2002

The effects of the first nonlinear corrections to the DGLAP evolution equations are studied by using the recent HERA data for the structure function $F_2(x,Q^2)$ of the free proton and the parton distributions from CTEQ5L and CTEQ6L as a baseline. By requiring a good fit to the H1 data, we determine initial parton distributions at $Q_0^2=1.4$ GeV$^2$ for the nonlinear scale evolution. We show that the nonlinear corrections improve the agreement with the $F_2(x,Q^2)$ data in the region of $x\sim 3\cdot 10^{-5}$ and $Q^2\sim 1.5$ GeV$^2$ without paying the price of obtaining a worse agreement at larger values of $x$ and $Q^2$. For the gluon distribution the nonlinear effects are found to play…

PhysicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsFOS: Physical sciencesPartonScale (descriptive set theory)HERA01 natural sciencesGluonHigh Energy Physics - PhenomenologyNonlinear systemHigh Energy Physics - Phenomenology (hep-ph)Distribution (mathematics)DGLAP0103 physical sciences010306 general physicsParticle Physics - Phenomenology
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