Search results for "J-Psi"

showing 3 items of 3 documents

Measurement of Upsilon production in collisions at root s=2.76 TeV

2014

The production of Υ(1S) , Υ(2S) and Υ(3S) mesons decaying into the dimuon final state is studied with the LHCb detector using a data sample corresponding to an integrated luminosity of 3.3pb-1 collected in proton–proton collisions at a centre-of-mass energy of s=2.76  TeV. The differential production cross-sections times dimuon branching fractions are measured as functions of the Υ transverse momentum and rapidity, over the ranges pT<15 GeV/ c and 2.0<y<4.5 . The total cross-sections in this kinematic region, assuming unpolarised production, are measured to be σpp→Υ(1S)X×BΥ(1S)→μ+μ-=1.111±0.043±0.044nb,σpp→Υ(2S)X×BΥ(2S)→μ+μ-=0.264±0.023±0.011nb,σpp→Υ(3S)X×BΥ(3S)→μ+μ-=0.159±0.020±0.…

PP COLLISIONSScience & Technology530 PhysicsPhysicsPHYSICS PARTICLES & FIELDSOCTET QUARKONIA PRODUCTIONPhysics InstituteLHCb - Abteilung HofmannJ-PSIoctet quarkonia productin; PP collisions; J-PSI; hadronic production; decay; distributions; toolHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnuclearePhysical SciencesDISTRIBUTIONSTOOLFísica nuclearDECAYParticle Physics - ExperimentHADRONIC PRODUCTION
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First measurement of f′2 (1525) production in Z0 hadronic decays

1996

The inclusive production of the f(2)'(1525) in hadronic Z(0) decays has been studied in data collected by the DELPHI detector at LEP. The Ring Imaging Cherenkov detectors were important tools in the identification of the decay f(2)'(1525) --> K+K-. The average number of f(2)(')(1525) produced per hadronic Z decay, [f(2)'] = 0.020 +/- 0.005 (stat) +/- 0.006 (syst), and the momentum distribution of the f(2)'(1525) have both been measured. The mass and width of the f(2)'(1525) are found to be [M(f2)'] = 1535 +/- 5 (stat) +/- 4 (syst) MeV/c(2). [Gamma(f2)'] = 60 +/- 20 (stat) +/- 19 (syst) MeV/c(2)

Nuclear and High Energy PhysicsLUND MONTE-CARLOCherenkov detectorElectron–positron annihilationK+KHadron01 natural sciencesPartícules (Física nuclear)JET FRAGMENTATIONPrime (order theory)law.inventionK identificationMomentumNuclear physicslaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment010306 general physicsCherenkov radiationDELPHIPhysicsDELPHI; Cherenkov detector; K identificationE+E-PHYSICS010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyJ-PSILARGE ELECTRON POSITRON COLLIDERSTATESPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentProduction (computer science)Particle Physics - ExperimentCherenkov detectorLUND MONTE-CARLO; JET FRAGMENTATION; E+E-PHYSICS; J-PSI; STATES; K+K
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Measurement of upsilon production in 7 TeV pp collisions at ATLAS

2013

Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UAM

Prompt J/Psi ProductionUpsilon meson01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Polarization[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQCQuantum chromodynamicsPhysicsLarge Hadron ColliderHeavy QuarkoniumSettore FIS/01 - Fisica SperimentaleCharmonium ProductionATLASJ-PsiHelicityLarge Hadron ColliderHadronic CollisionsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCpp collisionsParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsMesonCiências Naturais::Ciências Físicas530 PhysicsGluons:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2upsilon production; pp collisions ; ATLAS; detector530Nuclear physics0103 physical sciencesddc:530RapidityHigh Energy Physics010306 general physicsScience & TechnologyATLAS detector010308 nuclear & particles physicsBranching fractionFísicaQCDGluonOctet Quarkonia ProductionHADRON-HADRON COLLISIONSRoot-S=7 TevExperimental High Energy PhysicsHigh Energy Physics::ExperimentHeavy quarkonia
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