Search results for "transverse [mass]"

showing 10 items of 1055 documents

"Table 4" of "Transverse momentum of J / psi produced in p Cu, p U, O-16 Cu, O-16 U and S-32 U collisions at 200-GeV per nucleon."

1991

CONTINUUM MUONS ORIGINATE MAINLY FROM VECTOR MESON DECAYS, SEMI-LEPTONIC DECAYS OF D DBAR PAIRS AND FROM DRELL-YAN MECHANISM.

Di-Muon ProductionNuclear TheoryHigh Energy Physics::PhenomenologyMathematics::General TopologyO16 CU --> MU- MU+ (NEUTRALS) XMuon productionJ/PsiInclusiveSingle Differential Cross SectionNUCLEUS NUCLEUS --> (NEUTRALS) MU+ MU- XHigh Energy Physics::ExperimentDSIG/DPTPsiNuclear ExperimentTransverse Momentum DependenceDrell Yan
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"Table 3" 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 2.5

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringP P --> BOTTOM BOTTOMBAR XHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
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"Table 1" 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 2.5

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringP P --> BOTTOM BOTTOMBAR XHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
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"Table 6" 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 3.4

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringP P --> BOTTOM BOTTOMBAR XHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
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"Table 5" 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 3.1

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringP P --> BOTTOM BOTTOMBAR XHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
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"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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Orlicz–Sobolev extensions and measure density condition

2010

Abstract We study the extension properties of Orlicz–Sobolev functions both in Euclidean spaces and in metric measure spaces equipped with a doubling measure. We show that a set E ⊂ R satisfying a measure density condition admits a bounded linear extension operator from the trace space W 1 , Ψ ( R n ) | E to W 1 , Ψ ( R n ) . Then we show that a domain, in which the Sobolev embedding theorem or a Poincare-type inequality holds, satisfies the measure density condition. It follows that the existence of a bounded, possibly non-linear extension operator or even the surjectivity of the trace operator implies the measure density condition and hence the existence of a bounded linear extension oper…

Discrete mathematicsTransverse measureComplete measureApplied MathematicsBounded functionComplex measureσ-finite measureMeasure (mathematics)AnalysisSobolev inequalityTrace operatorMathematicsJournal of Mathematical Analysis and Applications
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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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