Search results for "RAPIDITY"

showing 10 items of 810 documents

"Figure 8b-2" of "Ground and excited charmonium state production in p+p collisions at sqrt(s)=200 GeV"

2023

Transverse momentum dependence of $J/\psi$ and $\psi^{\prime}$ yields in $|y|$ < 0.35, and ${\psi^{\prime}}/{J/\psi}$ ratio together with ratios obtained in other experiments. Uncertainties are point-to-point uncorrelated (uncorr.) (statistical and uncorrelated systematic uncertainties) and correlated systematic (corr.) uncertainties. The global uncertainty is 10%.

dielectron decay$p$ $p$ --> CHARGED Xppg104midrapiditycharmonium measurements200.0
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"Table 15b" of "Ground and excited charmonium state production in p+p collisions at sqrt(s)=200 GeV"

2023

$J/\psi$ counts obtained from the dimuon decay analysis of four different data sets, determined using the fit function. The S and N following 2006 and 2008 indicate the data sets for the south and north forward arms.

dielectron decay$p$ $p$ --> CHARGED Xppg104midrapiditycharmonium measurements200.0
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"Table 6a" of "Ground and excited charmonium state production in p+p collisions at sqrt(s)=200 GeV"

2023

$\psi^{\prime}(J/\psi)$ dielectron yield ratio measured at $|y|$ < 0.35 followed by point-to-point uncorrelated (uncorr.) (statistical and uncorrelated systematic uncertainties) and correlated systematic (corr.) uncertainties.

dielectron decay$p$ $p$ --> CHARGED Xppg104midrapiditycharmonium measurements200.0
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"Figure 21" of "Ground and excited charmonium state production in p+p collisions at sqrt(s)=200 GeV"

2023

Rapidity dependence of the $J/\psi$ yield combining dielectron ($|y|$ < 0.35 - full squares) with dimuon channels (1.2 < $|y|$ < 2.4 - full circles) along with the fits used to estimate the total cross section. Uncertainties are point-to-point uncorrelated (uncorr.) (statistical and uncorrelated systematic uncertainties) and correlated systematic (corr.) uncertainties. The global uncertainty is 10%.

dielectron decay$p$ $p$ --> CHARGED Xppg104midrapiditycharmonium measurements200.0
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"Figure 8a" of "Ground and excited charmonium state production in p+p collisions at sqrt(s)=200 GeV"

2023

Transverse momentum dependence of $J/\psi$ and $\psi^{\prime}$ yields in $|y|$ < 0.35, and ${\psi^{\prime}}/{J/\psi}$ ratio together with ratios obtained in other experiments. Uncertainties are point-to-point uncorrelated (uncorr.) (statistical and uncorrelated systematic uncertainties) and correlated systematic (corr.) uncertainties. The global uncertainty is 10%.

dielectron decay$p$ $p$ --> CHARGED Xppg104midrapiditycharmonium measurements200.0
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Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC

2017

Physical review letters 118(16), 162302 (2017). doi:10.1103/PhysRevLett.118.162302

heavy ion: scattering:Kjerne- og elementærpartikkelfysikk: 431 [VDP]transverse momentum [correlation function]correlation [momentum]550Pb-PbPb-Pb collisionsGeneral Physics and Astronomyhiukkasfysiikkanucl-exPP01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ALICEDEPENDENCEddc:550Nuclear Experiment (nucl-ex)ROOT-S(NN)=2.76 TEVNuclear ExperimentPERSPECTIVENuclear ExperimentPhysics and Astronomy (all); ALICE; LHCPhysicscorrelation function: transverse momentumPhysicsflow ; transverse ; momentum ; Pb-Pbtransverse momentum: correlationtwo-particleHanbury-Brown-Twiss effect:Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]PRIRODNE ZNANOSTI. Fizika.transverseTransverse planeCorrelation function (statistical mechanics)CERN LHC Coll:Nuclear and elementary particle physics: 431 [VDP]flowPseudorapidityLHCParticle Physics - ExperimentdeconfinementParticle physicscollectiveVDP::Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431FOS: Physical sciencesmomentumtriangulationPhysics and Astronomy(all)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesBethe ansatzMomentumNuclear physicsCENTRALITYPhysics and Astronomy (all)statistical analysisFactorizationscattering [heavy ion]Relativistic heavy-ion collisions0103 physical sciencesALICE / ALICE2760 GeV-cmsNuclear Physics - ExperimentRapiditystructurenumerical calculations010306 general physicsNuclear Physicstwo-particle transverse momentum differential correlation functionAnsatzleadDEPENDENCE PERSPECTIVE CENTRALITY PP.ta114VDP::Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431hep-ex010308 nuclear & particles physics:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]momentum: correlationBethe ansatzROOT-S(NN)=2.76 TEV; DEPENDENCE; PERSPECTIVE; PPNATURAL SCIENCES. Physics.rapiditypile-uptransverse momentum: factorizationfactorization [transverse momentum]correlation [transverse momentum]experimental results
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Features of W production in p-p, p-Pb and Pb-Pb collisions

2017

We consider the production of inclusive W bosons in variety of high-energy hadronic collisions: p--p, p--$\overline{\rm p}$, p--Pb, and Pb--Pb. In particular, we focus on the resulting distributions of charged leptons from W decay that can be measured with relatively low backgrounds. The leading-order expressions within the collinearly factorized QCD indicate that the center-of-mass energy dependence at forward/backward rapidities should be well approximated by a simple power law. The scaling exponent is related to the small-$x$ behaviour of the quark distributions, which is largely driven by the parton evolution. An interesting consequence is the simple scaling law for the lepton charge as…

heavy ion: scatteringHadronPb-Pb collisionsPartonElementary particle02 engineering and technologycomputer.software_genrePower lawHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)background: lowHigh Energy Physics - Phenomenology (hep-ph)0202 electrical engineering electronic engineering information engineering[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]050107 human factorsBosonQuantum chromodynamicsPhysicsDatabasehigher-order: 0Hadronic collisionsCharge asymmetries05 social sciencesscalinghep-phCharged leptonsHigh Energy Physics - PhenomenologyCERN LHC CollParticle Physics - ExperimentQuarkInelastic scatteringParticle physicssmall-xquark: distribution functionp p: scatteringFOS: Physical sciencesW: decay114 Physical sciencesenergy dependence[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]W: productionquantum chromodynamicsanti-p p: scatteringCollision systems0501 psychology and cognitive sciencesHigh energy physicsp nucleus: scatteringBosonsParticle Physics - Phenomenologyhep-exlepton: charge: asymmetryfactorization: collinearHigh Energy Physics::PhenomenologyElementary particlesScaling exponent Lead alloys020207 software engineeringBinary alloysW bosonsLeading ordersrapidityevolution equation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentcomputerhigh-energy hadronic collisionsLead Center-of-mass energiesLepton
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First measurement of the |t|-dependence of coherent J/ψ photonuclear production

2021

The first measurement of the dependence on $|t|$, the square of the momentum transferred between the incoming and outgoing target nucleus, of coherent J/ψ photoproduction is presented. The data were measured with the ALICE detector in ultra-peripheral Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}} = 5.02$ TeV with the J/$\psi$ produced in the central rapidity region $|y| < 0.8$, which corresponds to the small Bjorken-$x$ range $(0.3 − 1.4) \times 10 ^{−3}$. The measured $|t|$-dependence is not described by computations based only on the Pb nuclear form factor, while the photonuclear cross section is better reproduced by models including shadowing according t…

heavy ion: scatteringnucleon: pairVDP::Matematikk og Naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431nucl-ex01 natural sciencesSquare (algebra)ALICEJ/psi(3100): photoproduction[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQuantum chromodynamicsPhysicsPhysicsForm factor (quantum field theory)ultra-peripheral collisionsdependence [impact parameter]J/psi ALICE Pb-Pb collisionsBalitsky-Kovchegov equationQuarkoniumddc:3. Good healthPHOTOPRODUCTIONshadowingNucleonParticle Physics - ExperimentPB-PB COLLISIONSNuclear and High Energy PhysicsQC1-999nucleus: form factor[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]MomentumNuclear physicsPHYSICSCross section (physics)heavy-ion collisions ultra-peripheral collisions quarkoniaphotoproduction [J/psi(3100)]scattering [heavy ion]0103 physical sciencesNuclear Physics - Experimentddc:530Rapidity5020 GeV-cms/nucleonHeavy Ion experiments010306 general physicsimpact parameter: dependencehep-ex010308 nuclear & particles physicsnucleus: targetpair [nucleon]photonuclear productionheavy-ion collisionsquarkoniaform factor [nucleus]PB-PB COLLISIONS; PHOTOPRODUCTION; PHYSICStarget [nucleus]J/PsicoherenceJ/psi(3100): photoproduction ; impact parameter: dependence ; nucleus: form factor ; nucleus: target ; nucleon: pair ; heavy ion: scattering ; coherence ; Balitsky-Kovchegov equation ; shadowing ; rapidity ; ALICE ; experimental results ; 5020 GeV-cms/nucleonrapidityphotonuclear production J/Psi Pb-Pb collisionsHigh Energy Physics::Experimentexperimental results
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High-energy resummation effects in the production of Mueller-Navelet dijet at the LHC

2016

We study the production of two forward jets with a large interval of rapidity at hadron colliders, which was proposed by Mueller and Navelet as a possible test of the high energy dynamics of QCD, within a complete next-to-leading logarithm framework. We show that using the Brodsky-Lepage-Mackenzie procedure to fix the renormalization scale leads to a very good description of the recent CMS data at the LHC for the azimuthal correlations of the jets. We show that the inclusion of next-to-leading order corrections to the jet vertex significantly reduces the importance of energy-momentum non-conservation which is inherent to the BFKL approach, for an asymmetric jet configuration. Finally, we ar…

jetsCOLLISIONSParticle physicsLogarithmQC1-999Hadronenergy-momentumFOS: Physical sciencesPartonPART114 Physical sciences01 natural sciencesrenormalizationHigh Energy Physics - ExperimentRenormalizationHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)RAPIDITY0103 physical sciencesSCATTERINGRapidityResummationPROBE010306 general physicsNLO JET VERTEXQCD POMERONBFKLPhysicsQuantum chromodynamicsliikeoppiLarge Hadron Colliderta114010308 nuclear & particles physicsPhysicsscatteringHigh Energy Physics::PhenomenologydijetHigh Energy Physics - PhenomenologykinematicsresummationTEVHigh Energy Physics::Experimentviolationhadronquantym chromodynamicsBDKL equationAPPROXIMATION
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"Figure 2" of "Measurement of jet-medium interactions via direct photon-hadron correlations in Au$+$Au and $d$$+$Au collisions at $\sqrt{s_{_{NN}}}=2…

2021

Per-trigger yield of hadrons associated to direct photons in Au+Au collisions for direct photon $p_T$ 5-9 GeV/$c$, compared with p+p baseline, in various $\xi$ bins.

mid-rapidityHigh Energy Physics::Experimenttransverse momentumNuclear Experimentppg210photon-hadron correlationsAU AU200.0
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