Search results for "Deep Inelastic Scattering"

showing 10 items of 429 documents

Inclusive cross section and double-helicity asymmetry forπ0production at midrapidity inp+pcollisions ats=510  GeV

2016

PHENIX measurements are presented for the cross section and double-helicity asymmetry (A(LL)) in inclusive pi(0) production at midrapidity from p + p collisions at root s = 510 GeV from data taken in 2012 and 2013 at the Relativistic Heavy Ion Collider. The next-to-leading-order perturbative-quantum-chromodynamics theory calculation is in excellent agreement with the presented cross section results. The calculation utilized parton-to-pion fragmentation functions from the recent DSS14 global analysis, which prefer a smaller gluon-to-pion fragmentation function. The pi(0)A(LL) results follow an increasingly positive asymmetry trend with p(T) and root s with respect to the predictions and are …

PhysicsParticle physics010308 nuclear & particles physicsmedia_common.quotation_subjectParticle acceleratorDeep inelastic scatteringPolarization (waves)01 natural sciencesHelicityAsymmetrylaw.inventionGluonNuclear physicslaw0103 physical sciencesPiHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsRelativistic Heavy Ion Collidermedia_commonPhysical Review D
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EPS09 - Global NLO analysis of nuclear PDFs

2009

In this talk, we present our recent work on next-to-leading order (NLO) nuclear parton distribution functions (nPDFs), which we call EPS09. As an extension to earlier NLO analyses, we complement the deep inelastic scattering and Drell-Yan dilepton data by inclusive midrapidity pion production measurements from RHIC to reduce the otherwize large freedom of the nuclear gluon densities. In addition, our Hessian-type error analysis leading to a collection of nPDF error sets, is the first of its kind among the nPDF analyses.

PhysicsParticle physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::PhenomenologyNuclear TheoryDrell–Yan processFOS: Physical sciencesStatistical analysisHigh Energy Physics::ExperimentDeep inelastic scatteringNuclear Experiment
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Electron-ion physics with the LHeC

2015

The Large Hadron Electron Collider (LHeC) project is the proposal to use the existing LHC proton/ion beams and construct a new electron beam line to perform high-energy electron-proton/ion collisions. In this talk, we consider some of the physics topics that could be studied in the electron-ion mode. In particular, we estimate how much the current nuclear parton distribution fits could be improved with the deeply inelastic scattering measurements at the LHeC by including pseudodata into a global analysis. In addition, we discuss briefly other topics that would help to better understand some aspects of heavy-ion collisions, namely small-$x$ physics and hadron production with a nuclear target.

PhysicsParticle physicsLarge Hadron ColliderProton010308 nuclear & particles physicsHadronFOS: Physical sciencesPartonElectronInelastic scatteringDeep inelastic scattering01 natural scienceslaw.inventionNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawelectron-ion physics0103 physical sciencesLHeCLarge Hadron Electron Collider project010306 general physicsColliderNuclear Experiment
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Nonperturbative-transverse-momentum effects and evolution in dihadron and direct photon-hadron angular correlations in p+p collisions at s=510  GeV

2017

Dihadron and isolated direct photon-hadron angular correlations are measured in $p$$+$$p$ collisions at $\sqrt{s}=510$ GeV. Correlations of charged hadrons of $0.7<p_T<10$ GeV/$c$ with $\pi^0$ mesons of $4<p_T<15$ GeV/$c$ or isolated direct photons of $7<p_T<15$ GeV/$c$ are used to study nonperturbative effects generated by initial-state partonic transverse momentum and final-state transverse momentum from fragmentation. The nonperturbative behavior is characterized by measuring the out-of-plane transverse momentum component $p_{\rm out}$ perpendicular to the axis of the trigger particle, which is the high-$p_T$ direct photon or $\pi^0$. Nonperturbative evolution effects are extracted from …

PhysicsParticle physicsPhotonMeson010308 nuclear & particles physicsScatteringHadronDrell–Yan processDeep inelastic scattering01 natural sciencesRoot mean squareNuclear physicsFactorization0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review D
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Nucleon resonance contributions to unpolarised inclusive electron scattering

2019

The first CLAS12 experiments will provide high-precision data on inclusive electron scattering observables at a photon virtuality Q2 ranging from 0.05 to 12GeV2 and center-of-mass energies W up to 4 GeV. In view of this endeavor, we present the modeling of the resonant contributions to the inclusive electron scattering observables. As input, we use the existing CLAS electrocoupling results obtained from exclusive meson electroproduction data off protons, and evaluate for the first time the resonant contributions based on the experimental results on the nucleon resonance electroexcitation. The uncertainties are given by the data and duly propagated through a Monte Carlo approach. In this way…

PhysicsParticle physicsPhotondeep inelastic scattering; proton structureNuclear TheoryMeson010308 nuclear & particles physicsMonte Carlo methodNuclear TheoryFOS: Physical sciencesPartonObservable01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsNucleonNuclear ExperimentNuclear theoryElectron scatteringproton structure
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The spin structure of the nucleon

2005

An introduction to deep inelastic scattering experiments investigating the spin structure of the proton and the neutron is given. Discussed are measurements with longitudinally polarized targets to determine the spin structure functiong 1 and sum rules and to do pQCD analyses with inclusive data, while a flavour separation and first extractions of the gluon polarization are performed with semi-inclusive data.

PhysicsParticle physicsSpin polarizationDynamic structure factorNuclear TheoryGeneral Physics and AstronomySpin structureInelastic scatteringDeep inelastic scatteringGluonNuclear physicsHigh Energy Physics::ExperimentNeutronNuclear ExperimentNucleonCzechoslovak Journal of Physics
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nPDF constraints from the large hadron electron collider

2016

An updated analysis regarding the expected nuclear PDF constraints from the future Large Hadron Electron Collider (LHeC) experiment is presented. The new study is based on a more flexible small-$x$ parametrization which provides less biased uncertainty estimates in the region where there are currently no data constraints. The effect of the LHeC is quantified by directly including a sample of pseudodata according to the expected precision of this planned experiment. As a result, a significant reduction of the small-$x$ uncertainties in sea quarks and gluons is observed.

PhysicsParticle physicsparton distribution functions05 social sciencesHadronnuclear collisionsFOS: Physical sciences020207 software engineering02 engineering and technologyElectronDeep inelastic scatteringlaw.inventionNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawQuark–gluon plasma0202 electrical engineering electronic engineering information engineering0501 psychology and cognitive sciencesColliderParametrization050107 human factorsProceedings of XXIV International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS2016)
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The spin-dependent structure function g1(x) of the proton from polarized deep-inelastic muon scattering

1997

We present a new measurement of the virtual photon proton asymmetry $A_1^{\rm p}$ from deep inelastic scattering of polarized muons on polarized protons in the kinematic range $0.0008 1$ GeV$^{2}$. A perturbative QCD evolution in next-to-leading order is used to determine $g_1^{\rm p}(x)$ at a constant $Q^2$. At $Q^{2} = 10$ GeV$^{2}$ we find, in the measured range, $\int_{0.003}^{0.7} g_{1}^{\rm p}(x){\rm d}x = 0.139 \pm 0.006~({\rm stat})\pm 0.008~({\rm syst)} \pm 0.006~({\rm evol})$. The value of the first moment $\Gamma_{1}^{\rm p} = \int_{0}^{1} g_{1}^{\rm p}(x){\rm d}x$ of $g_{1}^{\rm p}$ depends on the approach used to describe the behaviour of $g_{1}^{\rm p}$ at low $x$. We find tha…

PhysicsQuantum chromodynamicsDISNuclear and High Energy PhysicsParticle physicsMuonProtonSMCScatteringg1 structure functionSMC; DIS; g1 structure functionPerturbative QCDDeep inelastic scatteringNuclear physicsSum rule in quantum mechanicsNucleonParticle Physics - ExperimentPhysics Letters B
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How to perform QCD analysis of DIS in Analytic Perturbation Theory

2015

We apply (Fractional) Analytic Perturbation Theory (FAPT) to the QCD analysis of the nonsinglet nucleon structure function $F_2(x,Q^2)$ in deep inelastic scattering up to the next leading order and compare the results with ones obtained within the standard perturbation QCD. Based on a popular parameterization of the corresponding parton distribution we perform the analysis within the Jacobi Polynomial formalism and under the control of the numerical inverse Mellin transform. To reveal the main features of the FAPT two-loop approach, we consider a wide range of momentum transfer from high $Q^2\sim 100 {\rm GeV}^2$ to low $Q^2\sim 0.3 {\rm GeV}^2$ where the approach still works.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsMellin transformParticle physicsMomentum transferInverseFOS: Physical sciencesPartonDeep inelastic scatteringsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)symbolsJacobi polynomialsHigh Energy Physics::ExperimentNucleon
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Measurement of inclusive jet and dijet production inppcollisions ats=7  TeVusing the ATLAS detector

2012

Inclusive jet and dijet cross sections have been measured in proton-proton collisions at a centre-of-mass energy of 7 TeV using the ATLAS detector at the Large Hadron Collider. The cross sections were measured using jets clustered with the anti-kT algorithm with parameters R=0.4 and R=0.6. These measurements are based on the 2010 data sample, consisting of a total integrated luminosity of 37 inverse picobarns. Inclusive jet double-differential cross sections are presented as a function of jet transverse momentum, in bins of jet rapidity. Dijet double-differential cross sections are studied as a function of the dijet invariant mass, in bins of half the rapidity separation of the two leading …

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHadronPartonHERADeep inelastic scattering7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant massRapidity010306 general physicsPhysical Review D
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