Search results for "distribution function"

showing 10 items of 348 documents

Tau polarization at the Z peak from the acollinearity between both τ-decay products

1992

21 páginas, 4 figuras, 6 tablas.

PhysicsNuclear and High Energy PhysicsParticle physicsElectron–positron annihilationmedia_common.quotation_subjectElectroweak interactionFísicaElementary particleObservablePolarization (waves)AsymmetryNuclear physicsPionDistribution functionParticle Physics - Phenomenologymedia_commonNuclear Physics B
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Prospects for probing the gluon density in protons using heavy quarkonium hadroproduction

2001

We examine carefully bottomonia hadroproduction in proton colliders, especially focusing on the LHC, as a way of probing the gluon density in protons. To this end we develop some previous work, getting quantitative predictions and concluding that our proposal can be useful to perform consistency checks of the parameterization sets of different parton distribution functions.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderProtonNuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesPartonQuarkoniumGluonHigh Energy Physics - PhenomenologyDistribution functionHigh Energy Physics - Phenomenology (hep-ph)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment
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Measurement of the differential γ+c-jet cross section and the ratio of differential γ+c and γ+b cross sections in pp¯ collisions at s=1.96 TeV

2013

We present measurements of the differential cross section $d\sigma/dp_{T}^{\gamma}$ for the associated production of a $c$-quark jet and an isolated photon with rapidity $|y^{\gamma}| 15$ GeV. The cross section ratios $\sigma(\gamma+c)/\sigma(\gamma+b)$ as a function of $p_{T}^{\gamma}$ are also presented. The results are based on data corresponding to an integrated luminosity of 8.7 fb$^{-1}$ recorded with the D0 detector at the Fermilab Tevatron $p\bar{p}$ Collider at $\sqrt{s}=$1.96 TeV. The obtained results are compared to next-to-leading order perturbative QCD calculations using various parton distribution functions, to predictions based on the $k_{T}$-factorization approach, and to pr…

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaTevatronPerturbative QCDOrder (ring theory)Parton7. Clean energy01 natural sciencesNuclear physicsDistribution function0103 physical sciencesHigh Energy Physics::ExperimentRapidityProduction (computer science)010306 general physicsPhysics Letters B
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Measurement of the muon charge asymmetry from W boson decays

2008

We present a measurement of the muon charge asymmetry from W boson decays using 0.3 fb^{-1} of data collected at \sqrt{s}=1.96 GeV between 2002 and 2004 with the D0 detector at the Fermilab Tevatron ppbar Collider. We compare our findings with expectations from next-to-leading-order calculations performed using the CTEQ6.1M and MRST04 NLO parton distribution functions. Our findings can be used to constrain future parton distribution function fits.

PhysicsNuclear and High Energy PhysicsParticle physicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesCharge (physics)Parton01 natural sciencesHigh Energy Physics - Experimentlaw.inventionHigh Energy Physics - Experiment (hep-ex)Distribution functionlaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentFermilab010306 general physicsColliderNuclear ExperimentBoson
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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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Generalized parton distributions of the pion in a Bethe Salpeter approach

2004

We calculate generalized parton distribution functions in a field theoretic formalism using a covariant Bethe-Salpeter approach for the determination of the bound-state wave function. We describe the procedure in an exact calculation in scalar Electrodynamics proving that the relevant corrections outside our scheme vanish. We extend the formalism to the Nambu--Jona-Lasinio model, a realistic theory of the pion. We go in both cases beyond all previous calculations and discover that all important features required by general physical considerations, like symmetry properties, sum rules and the polynomiality condition, are explicitly verified. We perform a numerical study of their behavior in t…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryHigh Energy Physics::PhenomenologyScalar electrodynamicsFOS: Physical sciencesPartonNuclear Theory (nucl-th)Formalism (philosophy of mathematics)High Energy Physics - PhenomenologyPionDistribution functionHigh Energy Physics - Phenomenology (hep-ph)Strong couplingCovariant transformationFísica nuclearWave functionMathematical physics
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Measurement of the electron charge asymmetry inpp¯→W+X→eν+Xdecays inpp¯collisions ats=1.96  TeV

2015

We present a measurement of the electron charge asymmetry in $p\bar{p}\rightarrow W+X \rightarrow e\nu +X$ events at a center-of-mass energy of 1.96 TeV, using data corresponding to 9.7~fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider. The asymmetry is measured as a function of the electron pseudorapidity and is presented in five kinematic bins based on the electron transverse energy and the missing transverse energy in the event. The measured asymmetry is compared with next-to-leading-order predictions in perturbative quantum chromodynamics and provides accurate information for the determination of parton distribution functions of the prot…

PhysicsNuclear and High Energy PhysicsParticle physicsProtonmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronPartonElectron7. Clean energyAsymmetryNuclear physicsDistribution functionPseudorapidityHigh Energy Physics::ExperimentNuclear Experimentmedia_commonLeptonPhysical Review D
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A quark model analysis of the transversity distribution

1997

The feasibility of measuring chiral-odd parton distribution functions in polarized Drell-Yan and semi-inclusive experiments has renewed theoretical interest in their study. Models of hadron structure have proven succesful in describing the gross features of the chiral-even structure functions. Similar expectations support our study of the transversity parton distributions in the Isgur-Karl and MIT bag models. We confirm the diverse low x behavior of the transversity and spin structure functions at the experimental scale and show that it is fundamentally a consequence of the different behavior under evolution of these functions. The inequalities of Soffer establish constraints between data a…

PhysicsNuclear and High Energy PhysicsParticle physicsQuark modelHadronStructure functionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPartonSpin structureHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution functionNuclear Experiment
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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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