Search results for "parton [model]"

showing 10 items of 214 documents

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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Can we fit nuclear PDFs with the high-x CLAS data?

2020

AbstractNuclear parton distribution functions (nuclear PDFs) are non-perturbative objects that encode the partonic behaviour of bound nucleons. To avoid potential higher-twist contributions, the data probing the high-x end of nuclear PDFs are sometimes left out from the global extractions despite their potential to constrain the fit parameters. In the present work we focus on the kinematic corner covered by the new high-x data measured by the CLAS/JLab collaboration. By using the Hessian re-weighting technique, we are able to quantitatively test the compatibility of these data with globally analyzed nuclear PDFs and explore the expected impact on the valence-quark distributions at high x. W…

Hessian matrixParticle physicsPhysics and Astronomy (miscellaneous)EMC effectNuclear TheoryFOS: Physical sciencesPartonlcsh:Astrophysicshiukkasfysiikka01 natural sciences114 Physical sciencessymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsNuclear ExperimentEngineering (miscellaneous)Physics010308 nuclear & particles physicsddc:530530 Physiknuclear parton distribution functions (nuclear PDFs)High Energy Physics - PhenomenologyDistribution functionsymbolslcsh:QC770-798Nucleonydinfysiikka
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Bayesian PDF reweighting meets the Hessian methods

2016

Volume: 273 New data coming from the LHC experiments have a potential to extend the current knowledge of parton distribution functions (PDFs). As a short cut to the cumbersome and time consuming task of performing a new PDF fit, re weighting methods have been proposed. In this talk, we introduce the so-called Hessian re-weighting, valid for PDF fits that carried out a Hessian error analysis, and compare it with the better-known Bayesian methods. We determine the existence of an agreement between the two approaches, and illustrate this using the inclusive jet production at the LHC. Peer reviewed

Hessian matrixPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Colliderta114parton distribution functionsJet (mathematics)010308 nuclear & particles physicsBayesian probabilityPartonJET DATAre-weighting methodsPROTON114 Physical sciences01 natural sciencesBayesian re-weightingsymbols.namesakeError analysisPARTON DISTRIBUTIONS0103 physical sciencessymbolsLHCHessian re-weighting010306 general physicsNuclear and Particle Physics Proceedings
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PDF reweighting in the Hessian matrix approach

2014

We introduce the Hessian reweighting of parton distribution functions (PDFs). Similarly to the better-known Bayesian methods, its purpose is to address the compatibility of new data and the quantitative modifications they induce within an existing set of PDFs. By construction, the method discussed here applies to the PDF fits that carried out a Hessian error analysis using a non-zero tolerance $\Delta\chi^2$. The principle is validated by considering a simple, transparent example. We are also able to establish an agreement with the Bayesian technique provided that the tolerance criterion is appropriately accounted for and that a purely exponential Bayesian likelihood is assumed. As a practi…

Hessian matrixPhysicsParticle physicsNuclear and High Energy PhysicsStatistical methodsta114Bayesian probabilityFOS: Physical sciencesPartonQCDExponential functionHigh Energy Physics - Experimentsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Distribution functionHigh Energy Physics - Phenomenology (hep-ph)Error analysissymbolsParton modelApplied mathematicsJournal of High Energy Physics
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Neutrino Structure Functions from GeV to EeV Energies

2023

The interpretation of present and future neutrino experiments requires accurate theoretical predictions for neutrino-nucleus scattering rates. Neutrino structure functions can be reliably evaluated in the deep-inelastic scattering regime within the perturbative QCD (pQCD) framework. At low momentum transfers ($Q^2 \le {\rm few}$ GeV$^2$), inelastic structure functions are however affected by large uncertainties which distort event rate predictions for neutrino energies $E_\nu$ up to the TeV scale. Here we present a determination of neutrino inelastic structure functions valid for the complete range of energies relevant for phenomenology, from the GeV region entering oscillation analyses to …

High Energy Astrophysical Phenomena (astro-ph.HE)Nuclear and High Energy Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyNuclear TheoryParton DistributionsFOS: Physical sciencesDeep Inelastic Scattering or Small-x PhysicsHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Neutrino InteractionsSDG 7 - Affordable and Clean EnergyNuclear Experiment (nucl-ex)Astrophysics - High Energy Astrophysical PhenomenaNuclear Experiment
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"Table 95" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ coll…

2019

$|{\cos{\theta}^{\star}}|$ absolute differential cross-section at parton level. The parton level phase-space is limited to the region $p_T^{t,1} > 500~$GeV, $p_T^{t,2} > 350~$GeV.

High Energy Physics::Phenomenology$|{\cos{\theta}^{\star}}|$High Energy Physics::Experimentparton levelPP -->$t\bar{t}$ ---> all-hadronicNuclear Experiment13000
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"Table 163" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

$H_{T}^{t\bar{t}}$ covariance matrix for the absolute differential cross-section at parton level

High Energy Physics::PhenomenologyHigh Energy Physics::Experimentparton levelPP -->$t\bar{t}$ ---> all-hadronicNuclear Experiment$H_{T}^{t\bar{t}}$13000
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"Table 155" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

$|{p_{out}}^{t\bar{t}}|$ covariance matrix for the absolute differential cross-section at parton level

High Energy Physics::PhenomenologyHigh Energy Physics::Experimentparton levelPP -->$t\bar{t}$ ---> all-hadronicNuclear Experiment13000$|{p_{out}}^{t\bar{t}}|$
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"Table 162" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

${\Delta\phi}(t_1,t_2)$ correlation matrix for the normalized differential cross-section at parton level

High Energy Physics::PhenomenologyMathematics::General TopologyHigh Energy Physics::Experimentparton levelPP -->$t\bar{t}$ ---> all-hadronicNuclear Experiment${\Delta\phi}(t_1t_2)$13000
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"Table 159" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

${\Delta\phi}(t_1,t_2)$ covariance matrix for the absolute differential cross-section at parton level

High Energy Physics::PhenomenologyMathematics::General TopologyHigh Energy Physics::Experimentparton levelPP -->$t\bar{t}$ ---> all-hadronicNuclear Experiment${\Delta\phi}(t_1t_2)$13000
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