Search results for "Fragmentation function"

showing 10 items of 158 documents

"Table 62" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The ratio of the D(z) in different centrality intervals in PbPb and in pp for 199.53 < pTjet < 251.19 and 0.8 < eta < 1.2.

PB PB --> JETS XPbPb) / D(z5020.0pp)D(zp p --> JETS Xjet fragmentation functions
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"Table 70" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2019

The ratio of the D(z) in different centrality intervals in PbPb and in pp for 199.53 < pTjet < 251.19 and 0.0 < eta < 2.1.

PB PB --> JETS XPbPb) / D(z5020.0pp)D(zp p --> JETS Xjet fragmentation functions
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"Table 2" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The ratio of the D(z) in different centrality intervals in PbPb and in pp for 126.00 < pTjet < 158.49 and 0.0 < eta < 2.1.

PB PB --> JETS XPbPb) / D(z5020.0pp)D(zp p --> JETS Xjet fragmentation functions
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"Table 42" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The ratio of the D(z) in different centrality intervals in PbPb and in pp for 158.49 < pTjet < 199.53 and 0.3 < eta < 0.8.

PB PB --> JETS XPbPb) / D(z5020.0pp)D(zp p --> JETS Xjet fragmentation functions
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"Table 38" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The ratio of the D(z) in different centrality intervals in PbPb and in pp for 158.49 < pTjet < 199.53 and 0.0 < eta < 0.3.

PB PB --> JETS XPbPb) / D(z5020.0pp)D(zp p --> JETS Xjet fragmentation functions
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"Table 82" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The ratio of the D(z) in different centrality intervals in PbPb and in pp for 251.19 < pTjet < 316.22 and 1.2 < eta < 2.1.

PB PB --> JETS XPbPb) / D(z5020.0pp)D(zp p --> JETS Xjet fragmentation functions
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Probing the small- x nuclear gluon distributions with isolated photons at forward rapidities in p+Pb collisions at the LHC

2014

Inclusive direct photon production in p+Pb collisions at the LHC is studied within the NLO perturbative QCD. Our aim is to quantify the dominant $x$ regions probed at different rapidities and to identify the best conditions for testing the nuclear gluon parton distribution functions (nPDFs) at small $x$. A comparison to the inclusive pion production reveals that from these two processes the photons carry more sensitivity to the small-$x$ partons and that this sensitivity can be further increased by imposing an isolation cut for the photon events. The details of the isolation criteria, however, seem to make only a small difference to the studied $x$ sensitivity and have practically no effect…

Particle physicsNuclear and High Energy PhysicsPhotonmedia_common.quotation_subjectFRAGMENTATION FUNCTIONSeducationFOS: Physical sciencesPREDICTIONSPartonPROTONAsymmetry114 Physical sciencesPionHigh Energy Physics - Phenomenology (hep-ph)PERTURBATIVE QCDSCATTERINGHadronic CollidersNuclear Experimentmedia_commonPhysicsBOSON PRODUCTIONPROMPT PHOTONLarge Hadron Colliderta114QUARKPerturbative QCDHeavy Ion PhenomenologyGluonHigh Energy Physics - PhenomenologyDistribution functionPARTON DISTRIBUTIONSHigh Energy Physics::ExperimentPDFSJHEP
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Measurement of the jet fragmentation function and transverse profile in proton-proton collisions at a center-of-mass energy of 7 TeV with the ATLAS d…

2011

The jet fragmentation function and transverse profile for jets with 25 GeV<pT jet<500 GeV and |ηjet|<1.2 produced in proton–proton collisions with a center-of-mass energy of 7 TeV are presented. The measurement is performed using data with an integrated luminosity of 36 pb−1. Jets are reconstructed and their momentum measured using calorimetric information. The momenta of the charged particle constituents are measured using the tracking system. The distributions corrected for detector effects are compared with various Monte Carlo event generators and generator tunes. Several of these choices show good agreement with the measured fragmentation function. None of these choices reproduce both t…

Physics and Astronomy (miscellaneous)Atlas detectorMonte Carlo methodKinematics7. Clean energy01 natural sciencesScaling ViolationsHigh Energy Physics - ExperimentScatteringHigh Energy Physics - Experiment (hep-ex)jet fragmentation[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentPhysicsSettore FIS/01 - Fisica SperimentaleDetectorATLASCharged particleTransverse planePhysical SciencesQuarkFísica nuclearDistributionsLHCParticle Physics - ExperimentParticle physics530 PhysicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]jet fragmentation function; proton–proton collisions; ATLAS detectorFOS: Physical sciencesAnnihilationddc:500.2530Nuclear physicsQ2 Dependence0103 physical sciencesFragmentation functionFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasHeraScience & TechnologyATLAS detector010308 nuclear & particles physicsFísicaQCDproton-proton collisionsHigh Energy Physics::Experiment
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Medium Modification of Jet Fragmentation inAu+AuCollisions atsNN=200  GeVMeasured in Direct Photon-Hadron Correlations

2013

The jet fragmentation function is measured with direct photon-hadron correlations in p + p and Au + Au collisions at root S-NN = 200 GeV. The P-T of the photon is an excellent approximation to the initial P-T of the jet and the ratio Z(T) = P-T(h)/P-T(gamma) is used as a proxy for the jet fragmentation function. A statistical subtraction is used to extract the direct photon-hadron yields in Au + Au collisions while a photon isolation cut is applied in p + p. I-AA, the ratio of hadron yield opposite the photon in Au + Au to that in p + p, indicates modification of the jet fragmentation function. Suppression, most likely due to energy loss in the medium, is seen at high Z(T). The associated h…

PhysicsEnergy lossPhoton010308 nuclear & particles physicsHadronGeneral Physics and Astronomy7. Clean energy01 natural sciencesNuclear physicsFragmentation (mass spectrometry)0103 physical sciencesFragmentation functionHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsPhysical Review Letters
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MEASUREMENT OF THE PRODUCTION-RATES OF ETA AND ETA' IN HADRONIC-Z DECAYS

1992

The decays eta --> gammagamma and eta' --> etapi+pi- have been observed in hadronic decays of the Z produced at LEP. The fragmentation functions of both the eta and eta' have been measured. The measured multiplicities for x > 0.1 are 0.298 +/- 0.023 +/- 0.021 and 0.068 +/- 0.018 +/- 0.016 for eta and eta' respectively. While the fragmentation function for the eta is fairly well described by the JETSET Monte Carlo, it is found that the production rate of the eta' is a factor of four less than the corresponding prediction.

PhysicsNuclear and High Energy PhysicsParticle physicsE+E ANNIHILATIONElectron–positron annihilationMonte Carlo methodHadronLEPNuclear physicsFragmentation (mass spectrometry)Fragmentation functionHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsNuclear ExperimentParticle Physics - ExperimentProduction rate
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