Search results for "Parton distribution"

showing 10 items of 65 documents

Mesure de la section efficace de l'électroproduction de photons à JLAB dans le but d'effectuer une Séparation Rosenbluth de la contribution DVCS

2014

The study of the inner structure of hadrons allows us to understand the nature of the interactions between partons, quarks and gluons, described by Quantum Chromodynamics. The elastic scattering reactions, which have been studied in order to measure the nucleon form factors, are included in this frame. The inelastic scattering reactions are also included in this frame, they allow us to obtain information about the nucleon structure thanks to the development of the parton distribution functions (PDFs). While through elastic scattering we can obtain information about the charge distribution of the nucleon, and hence, about the spatial distribution of the partons, through inelastic scattering …

Jefferson Lab (CEBAF)Réactions exclusivesDeeply Virtual Compton Scattering (DVCS)Structure du nucléonNucleon structureElectromagnetic probefísica de partículasGeneralized Parton Distributions (GPDs)Exclusive reactions[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Diffusion Compton Profondément Virtuelle (DVCS)Sonde électromagnétiqueHigh Energy Physics::Experimentfísica de altas energíasNuclear ExperimentDistributions de partons généralisées (GPDs)
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Poopćene raspodjele partona i struktura sastavnog kvarka

2003

In a scenario where the constituent quarks are composite systems, generalized parton distributions (GPDs) are built from wave functions to be evaluated in a constituent quark model (CQM), convoluted with the GPDs of the constituent quarks themselves. The approach permits to access the full kinematical range corresponding to the DGLAP and ERBL regions, so that cross-sections for deeply virtual Compton scattering can be estimated.

Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics::Phenomenologyhard exclusive processes; constituent quarks; generalized parton distributions; deeply virtual Compton scatteringFOS: Physical sciencesHigh Energy Physics::ExperimentNuclear Experiment
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Measurement of azimuthal asymmetries associated with deeply virtual Compton scattering on a longitudinally polarized deuterium target

2010

Azimuthal asymmetries in exclusive electroproduction of a real photon from a longitudinally polarized deuterium target are measured with respect to target polarization alone and with respect to target polarization combined with beam helicity and/or beam charge. The asymmetries appear in the distribution of the real photons in the azimuthal angle $\phi$ around the virtual photon direction, relative to the lepton scattering plane. The asymmetries arise from the deeply virtual Compton scattering process and its interference with the Bethe-Heitler process. The results for the beam-charge and beam-helicity asymmetries from a tensor polarized deuterium target with vanishing vector polarization ar…

Nuclear and High Energy Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyEVOLUTION KERNELS010308 nuclear & particles physicsGENERALIZED PARTON DISTRIBUTIONS; IMPACT PARAMETER SPACE; ELECTRON STORAGE-RING; EVOLUTION KERNELS; HERA; SPIN; NUCLEON; QCDHERAIMPACT PARAMETER SPACEFOS: Physical sciencesQCD01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ELECTRON STORAGE-RINGSPINGENERALIZED PARTON DISTRIBUTIONS0103 physical sciencesddc:530High Energy Physics::ExperimentSDG 7 - Affordable and Clean EnergyNUCLEON010306 general physics
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Revisiting the D-meson hadroproduction in general-mass variable flavour number scheme

2018

We introduce a novel realization of the open heavy-flavour hadroproduction in general-mass variable flavour number scheme at next-to-leading order in perturbative QCD. The principal novelty with respect to the earlier works is in the treatment of small-transverse-momentum limit, which has been a particularly challenging kinematic region in the past. We show that by a suitable choice of scheme, it is possible to obtain a well-behaved description of the open heavy-flavour hadroproduction cross sections from zero up to asymptotically high transverse momentum. We contrast our calculation with the available D$^0$-meson data as measured by the LHCb and ALICE collaborations at the LHC, finding a v…

Nuclear and High Energy PhysicsParticle physicsFRAGMENTATION FUNCTIONSFlavourFOS: Physical sciences114 Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)HEAVY-QUARK PRODUCTION0103 physical sciencesD mesonSCATTERINGlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNUCLEAR COLLISIONSLimit (mathematics)QCD ANALYSIS010306 general physicsVariable (mathematics)PhysicsLarge Hadron Colliderta114010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyContrast (statistics)Perturbative QCDQCD phenomenologyHigh Energy Physics - PhenomenologyPARTON DISTRIBUTIONSlcsh:QC770-798High Energy Physics::ExperimentLHCHADRON-COLLISIONSMATTERRealization (systems)TO-LEADING ORDER
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Distribution Amplitudes of Heavy-Light Mesons

2019

A symmetry-preserving approach to the continuum bound-state problem in quantum field theory is used to calculate the masses, leptonic decay constants and light-front distribution amplitudes of empirically accessible heavy-light mesons. The inverse moment of the $B$-meson distribution is particularly important in treatments of exclusive $B$-decays using effective field theory and the factorisation formalism; and its value is therefore computed: $\lambda_B(\zeta = 2\,{\rm GeV}) = 0.54(3)\,$GeV. As an example and in anticipation of precision measurements at new-generation $B$-factories, the branching fraction for the rare $B\to \gamma(E_\gamma) \ell \nu_\ell$ radiative decay is also calculated…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaInverseFOS: Physical sciencesHeavy-light mesons01 natural sciencesParton distribution amplitudesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBound stateNonperturbative continuum methods in quantum field theoryEffective field theoryQuantum field theory010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsBranching fractionHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyB-meson decayslcsh:QC1-999High Energy Physics - PhenomenologyAmplitudeHigh Energy Physics::Experimentlcsh:PhysicsQuantum chromodynamics
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Status of nuclear PDFs after the first LHC p–Pb run

2017

In this talk, I overview the recent progress on the global analysis of nuclear parton distribution functions (nuclear PDFs). After first introducing the contemporary fits, the analysis procedures are quickly recalled and the ambiguities in the use of experimental data outlined. Various nuclear-PDF parametrizations are compared and the main differences explained. The effects of nuclear PDFs in the LHC p-Pb hard-process observables are discussed and some future prospects sketched.

Nuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciences114 Physical scienceshigh-energy nuclear collisionsHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentHigh-energy nuclear collisions nuclear parton distribution functionsNuclear theoryQuantum chromodynamicsPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicsObservableHigh Energy Physics - Phenomenologynuclear parton distribution functionsDistribution functionParametrization
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Search for the Standard Model Higgs boson in the two photon decay channel with the ATLAS detector at the LHC

2011

A search for the Standard Model Higgs boson in the two photon decay channel is reported, using 1.08 fb−11.08 fb[superscript −1] of proton–proton collision data at a centre-of-mass energy of 7 TeV recorded by the ATLAS detector. No significant excess is observed in the investigated mass range of 110–150 GeV. Upper limits on the cross-section times branching ratio of between 2.0 and 5.8 times the Standard Model prediction are derived for this mass range.

Nuclear and High Energy PhysicsParticle physicsPhotonFOS: Physical sciencesElementary particleFotonesddc:500.201 natural sciencesMassless Particles530Nnlo QCDHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Grand Unified Theoryddc:530CollisionsHigh Energy Physics010306 general physicsNuclear ExperimentBosonPhysicsLarge Hadron ColliderATLAS detector010308 nuclear & particles physicsBranching fractionParton DistributionsSettore FIS/01 - Fisica SperimentaleFísicaATLASHadron CollidersMassless particleATLAS; LHC; Higgs bosonstandard model Higgs bosonHiggs bosonFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Nuclear-mass dependence of azimuthal beam-helicity and beam-charge asymmetries in deeply virtual Compton scattering

2009

The nuclear-mass dependence of azimuthal cross section asymmetries with respect to charge and longitudinal polarization of the lepton beam is studiedfor hard exclusive electroproduction of real photons. The observed beam-charge and beam-helicity asymmetries are attributed to the interference between the Bethe-Heitler and deeply virtual Compton scattering processes. For various nuclei, the asymmetries are extracted for both coherent and incoherent-enriched regions, which involve different (combinations of) generalized parton distributions. For both regions, the asymmetries are compared to those for a free proton, and no nuclear-mass dependence is found.

Nuclear and High Energy PhysicsParticle physicsPhotonNuclear TheoryHERAFOS: Physical sciencesIMPACT PARAMETER SPACEPartonGENERALIZED PARTON DISTRIBUTIONS; IMPACT PARAMETER SPACE; SPIN; HERA01 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)GENERALIZED PARTON DISTRIBUTIONS0103 physical sciencesddc:530Nuclear Experiment010306 general physicsPhysicsElastic scattering010308 nuclear & particles physicsScatteringCompton scatteringHERASPINPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNucleonBeam (structure)
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Pion-photon transition distribution amplitudes in the Nambu-Jona-Lasinio model

2007

12 pages, 6 figures.-- PACS nrs.: 13.60.-r; 11.10.St; 12.38.Lg; 24.10.Jv.-- ISI Article Identifier: 000251327200049.-- ArXiv pre-print available at: http://arxiv.org/abs/0707.3366

Nuclear and High Energy PhysicsPhotonBethe–Salpeter equationHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences[PACS] Relativistic models of nucleiPartícules (Física nuclear)PionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio modelBound stateVirtual Compton-scatteringCovariant transformation[PACS] Photon and charged-lepton interactions with hadrons[PACS] Bound and unstable statesMathematical physicsQuantum chromodynamicsPhysicsHigh Energy Physics::PhenomenologyGeneralized Parton distributions[PACS] Bound and unstable states; Bethe-Salpeter equations[PACS] Other nonperturbative calculations in QCDHigh Energy Physics - PhenomenologyAmplitudeQuantum electrodynamicsBethe-Salpeter equationsFísica nuclear
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Constraints on nuclear parton distributions from dijet photoproduction at the LHC

2019

Using QCD calculations of the cross section of inclusive dijet photoproduction in Pb-Pb ultraperipheral collisions in the LHC kinematics as pseudo-data, we study the effect of including these data using the Bayesian reweighting technique on nCTEQ15, nCTEQ15np, and EPPS16 nuclear parton distribution functions (nPDFs). We find that, depending on the assumed error of the pseudo-data, it leads to a significant reduction of the nPDF uncertainties at small values of the momentum fraction $x_A$. Taking the error to be 5\%, the uncertainty of nCTEQ15 and nCTEQ15np nPDFs reduces approximately by a factor of two at $x_A=10^{-3}$. At the same time, the reweighting effect on EPPS16 nPDFs is much smalle…

PB-PB COLLISIONSParticle physicsNuclear TheoryPhysics and Astronomy (miscellaneous)FOS: Physical scienceslcsh:AstrophysicsPartonhiukkasfysiikka114 Physical sciences01 natural sciencesCOLLIDERNuclear Theory (nucl-th)MomentumCross section (physics)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuantum ChromodynamicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentEngineering (miscellaneous)PhysicsQuantum chromodynamicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics - Phenomenologynuclear parton distribution functionsDistribution functionlcsh:QC770-798ydinfysiikkaVECTOR-MESONSParametrization
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