Search results for "Transverse momentum"

showing 10 items of 1015 documents

"Table 4" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

2012

pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 2.8

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyP P --> BOTTOM BOTTOMBAR < MU+ X > X7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
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First Measurement of Transverse-Spin-Dependent Azimuthal Asymmetries in the Drell-Yan Process

2017

The first measurement of transverse-spin-dependent azimuthal asymmetries in the pion-induced Drell-Yan (DY) process is reported. We use the CERN SPS 190 GeV/$c$, $\pi^{-}$ beam and a transversely polarized ammonia target. Three azimuthal asymmetries giving access to different transverse-momentum-dependent (TMD) parton distribution functions (PDFs) are extracted using dimuon events with invariant mass between 4.3 GeV/$c^2$ and 8.5 GeV/$c^2$. The observed sign of the Sivers asymmetry is found to be consistent with the fundamental prediction of Quantum Chromodynamics (QCD) that the Sivers TMD PDFs extracted from DY have a sign opposite to the one extracted from semi-inclusive deep-inelastic sc…

Drell-Yan process550ComputerSystemsOrganization_COMPUTERSYSTEMIMPLEMENTATIONNuclear TheoryGeneral Physics and Astronomyparton: distribution functiontransverse momentum dependence01 natural sciencesCOMPASSHigh Energy Physics - ExperimentSivers functionHigh Energy Physics - Experiment (hep-ex)semi-inclusive reaction [deep inelastic scattering]High Energy Physics - Phenomenology (hep-ph)ddc:550[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimenttransversityPhysicsQuantum chromodynamics(muon+ muon-) [mass spectrum]Large Hadron Colliderdeep inelastic scattering: semi-inclusive reactionpolarized target: transverse190 GeV/ctransverse [polarized target]nucleonDrell–Yan processhep-phdimuon: mass spectrumAzimuthHigh Energy Physics - PhenomenologyTransverse planeasymmetry [angular distribution]pi- nucleus: scatteringmass spectrum [dimuon]distribution function [parton]Nucleonspin: asymmetryParticle Physics - ExperimentParticle physicsangular distribution: asymmetryscattering [pi- nucleus]ComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONFOS: Physical sciencesComputerApplications_COMPUTERSINOTHERSYSTEMSAccelerator Physics and InstrumentationGeneralLiterature_MISCELLANEOUSNuclear physicsPhysics and Astronomy (all)[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciencesquantum chromodynamicsuniversality010306 general physicsParticle Physics - Phenomenology010308 nuclear & particles physicshep-exHigh Energy Physics::PhenomenologyAcceleratorfysik och instrumenteringCERN SPSmass spectrum: (muon+ muon-)ComputingMethodologies_PATTERNRECOGNITION[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Physics::Accelerator Physics[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentasymmetry [spin]experimental results
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Matching factorization theorems with an inverse-error weighting

2018

We propose a new fast method to match factorization theorems applicable in different kinematical regions, such as the transverse-momentum-dependent and the collinear factorization theorems in Quantum Chromodynamics. At variance with well-known approaches relying on their simple addition and subsequent subtraction of double-counted contributions, ours simply builds on their weighting using the theory uncertainties deduced from the factorization theorems themselves. This allows us to estimate the unknown complete matched cross section from an inverse-error-weighted average. The method is simple and provides an evaluation of the theoretical uncertainty of the matched cross section associated w…

Drell-Yan processNuclear and High Energy PhysicsFOS: Physical sciencesInversegauge boson: hadroproduction01 natural sciencestransverse momentum: momentum spectrumCross section (physics)High Energy Physics - Phenomenology (hep-ph)FactorizationfactorizationSimple (abstract algebra)0103 physical sciencesquantum chromodynamicsApplied mathematics010306 general physicshadron hadron: interactionBosonQuantum chromodynamicsPhysics010308 nuclear & particles physicsmatchingdeep-inelastic processesfactorization: collinearHigh Energy Physics::Phenomenologyfactorization; Quantum Chromodynamics; matching; power corrections; deep-inelastic processesDrell–Yan processlcsh:QC1-999WeightingHigh Energy Physics - Phenomenologykinematics[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]transverse momentum: factorization[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]power correctionslcsh:Physics
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Erratum to: DYTurbo: fast predictions for Drell–Yan processes

2020

The European physical journal / C 80(5), 440 (2020). doi:10.1140/epjc/s10052-020-7972-0

Drell-Yan processPhysics and Astronomy (miscellaneous)density [parton]Hadrontransverse momentum [resummation]Drell-YanParton01 natural sciencescorrelation [spin]colliding beams [hadron]pair production [lepton]ResummationHadron collidersPhysicsQuantum chromodynamicsprecision measurementhigher-order: 2resummation: transverse momentum2 [higher-order]kinematicsfactorization [cross section]parton: densityParticle physicsspin: correlation530 Physicslepton: pair productionlcsh:Astrophysics10192 Physics Institute530Standard Model0103 physical scienceslcsh:QB460-466quantum chromodynamicslcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:5303101 Physics and Astronomy (miscellaneous)010306 general physicsEngineering (miscellaneous)Electroweak010308 nuclear & particles physicshadron: colliding beamsHigh Energy Physics::PhenomenologyOrder (ring theory)cross section: factorizationQCDPair productionlcsh:QC770-798High Energy Physics::Experiment2201 Engineering (miscellaneous)Lepton
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DYTurbo: fast predictions for Drell–Yan processes

2019

The European physical journal / C 80(5), 251 (2020). doi:10.1140/epjc/s10052-020-7757-5

Drell-Yan processPhysics and Astronomy (miscellaneous)density [parton]transverse momentum [resummation]Drell-YanParton01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)correlation [spin]colliding beams [hadron]pair production [lepton]ResummationHadron collidersPhysicsQuantum chromodynamicsprecision measurementhigher-order: 2resummation: transverse momentumDrell–Yan processhep-ph2 [higher-order]High Energy Physics - Phenomenologykinematicsfactorization [cross section]parton: densityPhenomenology (particle physics)Particle physics530 Physicsspin: correlationlepton: pair productionFOS: Physical scienceslcsh:Astrophysics10192 Physics Institute530Standard Modellcsh:QB460-4660103 physical sciencesquantum chromodynamicsddc:530lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Particle Physics - PhenomenologyElectroweak010308 nuclear & particles physicshadron: colliding beamsHigh Energy Physics::Phenomenologycross section: factorizationQCDPair production[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]lcsh:QC770-798High Energy Physics::ExperimentLeptonThe European Physical Journal C
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Sivers asymmetry extracted in SIDIS at the hard scales of the Drell-Yan process at COMPASS

2017

Proton transverse-spin azimuthal asymmetries are extracted from the COMPASS 2010 semi-inclusive hadron measurements in deep inelastic muon-nucleon scattering in those four regions of the photon virtuality $Q^2$, which correspond to the four regions of the di-muon mass $\sqrt{Q^2}$ used in the ongoing analysis of the COMPASS Drell-Yan measurements. This allows for a future direct comparison of the nucleon transverse-momentum-dependent parton distribution functions extracted from these two alternative measurements. Various two-dimensional kinematic dependences are presented for the azimuthal asymmetries induced by the Sivers transverse-momentum-dependent parton distribution function. The inte…

Drellâ YanDrell-Yan processPhotonHadronparton: distribution functionDrell-YanPartontransverse momentum dependence01 natural sciencesCOMPASSSIDISHigh Energy Physics - ExperimentSivers functionSubatomär fysikHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)CompassSubatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]dimension: 2Nuclear ExperimentSIDIS; Drell–Yan; Spin; Azimuthal asymmetries; Sivers; TMDsmedia_commonPhysicsQuantum chromodynamicsdeep inelastic scattering: semi-inclusive reactionpolarized target: transversephotonDrell–Yan processhep-phlcsh:QC1-999Drell–YanAzimuthal asymmetrieHigh Energy Physics - PhenomenologykinematicsSiverpolarized beam: longitudinalNucleonAzimuthal asymmetriesspin: asymmetryParticle Physics - ExperimentParticle physicsNuclear and High Energy Physicsangular distribution: asymmetrymedia_common.quotation_subjectFOS: Physical sciencesTMDsAsymmetryNuclear physicsSpin[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]Azimuthal asymmetries; Drell–Yan; SIDIS; Sivers; Spin; TMDs; Nuclear and High Energy Physics0103 physical sciencesmuon nucleon: deep inelastic scatteringquantum chromodynamicsSiversmuon nucleon: scattering010306 general physicsParticle Physics - Phenomenologynucleon: transverse momentum010308 nuclear & particles physics160 GeV/chep-exCERN SPSmuon+ p: deep inelastic scattering[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentlcsh:Physicsexperimental results
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"Table 1" of "Inclusive cross sections, charge ratio and double-helicity asymmetries for $\pi^+$ and $\pi^-$ production in $p$$+$$p$ collisions at $\…

2016

Invariant cross section for $\pi^+$ and $\pi^-$ hadrons, as well as the statistical and systematic uncertainties. In addition, there is an absolute scale uncertainty of 9.6$\%$.

E*D3SIG/DP**3InclusiveSingle Differential Cross SectionProton-Proton ScatteringHigh Energy Physics::ExperimentDSIG/DPTP P --> PI+ XP P --> PI- XTransverse Momentum DependenceInvariant Cross Section200.0
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"Table 39" of "Properties of hadronic Z decays and test of QCD generators"

1992

Transverse momentum, PTOUT, distribution.

E+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringExclusive91.2Single Differential DistributionDN/DPTOUTNuclear ExperimentTransverse Momentum Dependence
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"Table 38" of "Properties of hadronic Z decays and test of QCD generators"

1992

Transverse momentum, PTOUT, distribution.

E+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringExclusive91.2Single Differential DistributionDN/DPTOUTNuclear ExperimentTransverse Momentum Dependence
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"Table 40" of "Properties of hadronic Z decays and test of QCD generators"

1992

Transverse momentum, PTIN, distribution.

E+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringExclusive91.2Single Differential DistributionNuclear ExperimentTransverse Momentum DependenceDN/DPTIN
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