Search results for "Inclusive"

showing 10 items of 5972 documents

"Table 2" of "Measurement of the correlations between the polar angles of leptons from top quark decays in the helicity basis at $\sqrt{s}=7$TeV usin…

2017

The correlation factors for the statistical uncertainties between any two bins of the unfolded distribution.

Quantitative Biology::BiomoleculesP P --> LEPTON+ NU LEPTON- NUBAR BOTTOM BOTTOMBAR XDifferential Cross SectionP P --> W+ W- BOTTOM BOTTOMBAR XTopTop Production7000.0Astrophysics::Cosmology and Extragalactic AstrophysicsPhysics::Data Analysis; Statistics and ProbabilityP P --> TOP TOPBAR XInclusiveProton-Proton ScatteringW Pair ProductionAngular DependenceW ProductionDSIG/DTHETA
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"Table 1" of "Measurement of the correlations between the polar angles of leptons from top quark decays in the helicity basis at $\sqrt{s}=7$TeV usin…

2017

The numerical summary of the unfolded $\cos\theta_1\cdot\cos\theta_2$ distribution, with statistical and systematic uncertainties.

Quantitative Biology::BiomoleculesStatistics::TheoryP P --> LEPTON+ NU LEPTON- NUBAR BOTTOM BOTTOMBAR XDifferential Cross SectionMathematics::History and OverviewP P --> W+ W- BOTTOM BOTTOMBAR XTopTop Production7000.0P P --> TOP TOPBAR XInclusiveProton-Proton ScatteringW Pair ProductionAngular DependenceW ProductionDSIG/DTHETA
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"Table 4" of "Flavour Separation of Helicity Distributions from Deep Inelastic Muon-Deuteron Scattering"

2010

The measured strange quark helicity distribution as a funxtion of X.

Quantitative Biology::BiomoleculesStrange productionHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryHELICITYDeep Inelastic ScatteringMuon productionMU+ DEUT --> MU+ K+ XInclusiveMU+ DEUT --> MU+ K- XNeutral Current140180Nuclear ExperimentMU+ DEUT --> MU+ X
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"Table 3" of "Flavour Separation of Helicity Distributions from Deep Inelastic Muon-Deuteron Scattering"

2010

Correlations coefficients of the unfolded asymmetries.

Quantitative Biology::BiomoleculesStrange productionMU+ DEUT --> MU+ PI+ XCORRDeep Inelastic ScatteringMuon productionMU+ DEUT --> MU+ K+ XInclusiveMU+ DEUT --> MU+ K- XNeutral CurrentHigh Energy Physics::Experiment140180MU+ DEUT --> MU+ PI- XMU+ DEUT --> MU+ X
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"Table 4" of "Search for dark matter in events with a hadronically decaying W or Z boson and missing transverse momentum in pp collisions at sqrt(s)=…

2014

Observed limits on the effective theory mass scale M* as a function of the dark matter mass M(chi) at 90% confidence-level from combined mono-W-boson and mono-Z-boson signals for various operators.

Quantitative Biology::Subcellular ProcessesCondensed Matter::Quantum GasesInclusive8000.0Proton-Proton ScatteringZ ProductionP P --> W- CHI CHIBAR XHigh Energy Physics::PhenomenologyP P --> Z0 CHI CHIBAR XMW ProductionP P --> W+ CHI CHIBAR X
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"Table 10" of "Search for new phenomena in events with a photon and missing transverse momentum in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS…

2015

Observed lower limits at 95% C.L. on the EFT suppression scale M* as a function of the mediator mass mV, for a Z'-like mediator with vector interactions. For a dark-matter mass m_chi of 50 or 400 GeV, results are shown for different values of the mediator total decay width Gamma.

Quantitative Biology::Subcellular ProcessesInclusive8000.0Proton-Proton ScatteringP P --> CHI CHI GAMMA XM
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Measurement of the chi(b) (3 P) mass and of the relative rate of chi(b1) (1 P) and chi(b2) (1 P) production

2014

The production of $\chi_b$ mesons in proton-proton collisions is studied using a data sample collected by the LHCb detector, at centre-of-mass energies of $\sqrt{s}=7$ and $8$ TeV and corresponding to an integrated luminosity of 3.0 fb$^{-1}$. The $\chi_b$ mesons are identified through their decays to $\Upsilon(1S)\gamma$ and $\Upsilon(2S)\gamma$ using photons that converted to $e^+e^-$ pairs in the detector. The $\chi_b(3P)$ meson mass, and the relative prompt production rate of $\chi_{b1}(1P)$ and $\chi_{b2}(1P)$ mesons as a function of the $\Upsilon(1S)$ transverse momentum in the $\chi_b$ rapidity range 2.0< $y$<4.5, are measured. Assuming a mass splitting between the $\chi_{b1}(3P)$ an…

Quantum chromodynamics: Experimental testPhysics::Instrumentation and DetectorsNuclear TheoryQuarkoniumFlavor physics; Hadron-Hadron Scattering; Quarkonium01 natural sciencesPhysics Particles & FieldsHigh Energy Physics - ExperimentLuminositySettore FIS/04 - Fisica Nucleare e Subnucleare14.40.PqFlavor physicsDECAY; UPSILON; PSI[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Flavor physics; Hadron-Hadron Scattering; Quarkonium; Nuclear and High Energy PhysicsPSINuclear ExperimentQCPhysicsPhysicsHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronParticle physicsLeptonic semileptonic and radiative decays of J/ψ Υ and other quarkoniaQuarkonium Hadron-Hadron Scattering Flavor physicsPhysical SciencesTransverse momentumFísica nuclearProduction (computer science)LHCParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsMesonLHCb - Abteilung HofmannAstrophysics::Cosmology and Extragalactic AstrophysicsUPSILONHadronsNO13.20.Gd0103 physical sciencesRapiditySDG 7 - Affordable and Clean Energy010306 general physicsLarge Hadron Collider (France and Switzerland)/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyScience & TechnologyHadron-Hadron Scattering010308 nuclear & particles physicsGran Col·lisionador d'HadronsLHCb12.38.QkFlavor physicHigh Energy Physics::ExperimentHeavy quarkonia13.85.NiFísica de partículesExperimentsDECAYProduction rate
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The internal structure of jets at colliders: light and heavy quark inclusive hadronic distributions

2010

In this paper, we report our results on charged hadron multiplicities of heavy quark initiated jets produced in high energy collisions. After implementing the so-called dead cone effect in QCD evolution equations, we find that the average multiplicity decreases significantly as compared to the massless case. Finally, we discuss on the transverse momentum distribution of light quark initiated jets and emphasize on the comparison between our predictions and CDF data.

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHadronmultiplicitiesStructure (category theory)General Physics and AstronomyFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesJets010306 general physicsNuclear ExperimentPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMultiplicity (mathematics)inclusive distributionsMassless particleHigh Energy Physics - PhenomenologyDistribution (mathematics)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Transverse momentumHigh Energy Physics::Experiment
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Single inclusive forward hadron production at next-to-leading order

2016

We discuss single inclusive hadron production from a high energy quark scattering off a strong target color field in the Color Glass Condensate formalism. Recent calculations of this process at the next-to-leading order accuracy have led to negative cross sections at large transverse momenta. We identify the origin of this problem as an oversubtraction of the rapidity divergence into the Balitsky-Kovchegov evolution equation for the target. We propose a new way to implement the kinematical restriction on the emitted gluons to overcome this difficulty.

QuarkParticle physicssingle inclusive hardon productionNuclear TheoryHadronFOS: Physical sciencescolor glass condensate formalism01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Balitsky-Kovchegov evolution0103 physical sciencesRapidityfysiikka010306 general physicsPhysicsta114010308 nuclear & particles physicsScatteringGluonTransverse planeHigh Energy Physics - PhenomenologyEvolution equationphysics
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Search for anomalous heavy-flavor quark production in association with W bosons.

2004

We present a search for anomalous production of heavy-flavor quark jets in association with a W boson at the Fermilab Tevatron ppbar Collider. This search is conducted through an examination of the exclusive jet spectrum of W+jets final states in which the heavy-flavor quark content has been enhanced by requiring at least one tagged jet in an event. Jets are tagged by the combined use of two algorithms, one based on semileptonic decays of b/c hadrons, and the other on their lifetimes. We compare data in e+jets (164 pb-1) and mu+jets (145 pb-1) channels, collected with the D0 detector at sqrt{s}=1.96 TeV, to expectations from the standard model, and set upper limits on anomalous production o…

Quarkflavour modelParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHadronstandard modelTevatronGeneral Physics and AstronomyFOS: Physical sciencesJet (particle physics)01 natural sciences7. Clean energyHigh Energy Physics - Experimentlaw.inventionStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilabquark production13.85.Qk 13.85.Nielementary particle jets010306 general physicsColliderBosonPhysicsproton-proton inclusive interactions010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyW bosonshigh-energy elementary particle interactionsHigh Energy Physics::ExperimentPhysical review letters
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