Search results for "Fragmentation function"

showing 10 items of 158 documents

"Table 37" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The D(pT) distributions in different centrality intervals in PbPb and in pp for 158.49 < pTjet < 199.53 and 0.0 < eta < 0.3.

5020.0PB PB --> JETS X(1/Nj)(dN/dpT)p p --> JETS Xjet fragmentation functions
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In-medium jet shape from energy collimation in parton showers: Comparison with CMS PbPb data at 2.76 TeV

2014

Abstract: We present the medium-modified energy collimation in the leading-logarithmic approximation (LLA) and next-to-leading-logarithmic approximation (NLLA) of QCD. As a consequence of more accurate kinematic considerations in the argument of the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) fragmentation functions (FFs) we find a new NLLA correction O ð α s Þ which accounts for the scaling violation of DGLAP FFs at small x . The jet shape is derived from the energy collimation within the same approximations and we also compare our calculations for the energy collimation with the event generators PYTHIA 6 and Y A JEM for the first time in this paper. The modification of jets by the …

Astrophysics::High Energy Astrophysical Phenomenacolor coherencefragmentation functionsHigh Energy Physics::Experimenthadron spectracollisions
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K− over K+ multiplicity ratio for kaons produced in DIS with a large fraction of the virtual-photon energy

2018

The K$^{-}$ over K$^{+}$ multiplicity ratio is measured in deep-inelastic scattering, for the first time for kaons carrying a large fraction $z$ of the virtual-photon energy. The data were obtained by the COMPASS collaboration using a 160 GeV muon beam and an isoscalar $^6$LiD target. The regime of deep-inelastic scattering is ensured by requiring $Q^2>1$ (GeV/$c)^2$ for the photon virtuality and $W>5$ GeV/$c^2$ for the invariant mass of the produced hadronic system. Kaons are identified in the momentum range from 12 GeV/$c$ to 40 GeV/$c$, thereby restricting the range in Bjorken-$x$ to $0.010.75$. For very large values of $z$, $i.e.$ $z>0.8$, we observe the kaon multiplicity ratio to fall …

Hadron0 [higher-order]target: isoscalar01 natural sciencesCOMPASSdeep inelastic scattering [muon+ nucleon]High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)K: multiplicityHigh Energy Physics - Phenomenology (hep-ph)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]isoscalar [target]Invariant massNuclear ExperimentBosonPhysicsQuantum chromodynamicsquark: fragmentation functionhigher-order: 0photonperturbation theory: higher-orderhep-phмюоныlcsh:QC1-999Bjorken [scaling]High Energy Physics - Phenomenologybeam [muon]рассеяниеfactorization [cross section]multiplicity [pi]Particle Physics - Experimentperturbation theory [quantum chromodynamics]Particle physicsNuclear and High Energy PhysicsMesonFOS: Physical sciencesratio [multiplicity]530fragmentation function [quark]x-dependencescaling: Bjorkencharged particle: multiplicityphase spacemultiplicity [charged particle][ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]виртуальные фотоны0103 physical sciencesddc:530universalityquantum chromodynamics: perturbation theory010306 general physicsParticle Physics - Phenomenologymuon+ nucleon: deep inelastic scatteringMuonmultiplicity: ratiopi: multiplicity010308 nuclear & particles physicshep-exmuon: beamMultiplicity (mathematics)cross section: factorizationCERN SPSDeep inelastic scatteringhigher-order [perturbation theory][PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]каоны[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentmultiplicity [K]hadronizationlcsh:Physicsexperimental resultsPhysics Letters B
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Revisiting the D-meson hadroproduction in general-mass variable flavour number scheme

2018

We introduce a novel realization of the open heavy-flavour hadroproduction in general-mass variable flavour number scheme at next-to-leading order in perturbative QCD. The principal novelty with respect to the earlier works is in the treatment of small-transverse-momentum limit, which has been a particularly challenging kinematic region in the past. We show that by a suitable choice of scheme, it is possible to obtain a well-behaved description of the open heavy-flavour hadroproduction cross sections from zero up to asymptotically high transverse momentum. We contrast our calculation with the available D$^0$-meson data as measured by the LHCb and ALICE collaborations at the LHC, finding a v…

Nuclear and High Energy PhysicsParticle physicsFRAGMENTATION FUNCTIONSFlavourFOS: Physical sciences114 Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)HEAVY-QUARK PRODUCTION0103 physical sciencesD mesonSCATTERINGlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNUCLEAR COLLISIONSLimit (mathematics)QCD ANALYSIS010306 general physicsVariable (mathematics)PhysicsLarge Hadron Colliderta114010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyContrast (statistics)Perturbative QCDQCD phenomenologyHigh Energy Physics - PhenomenologyPARTON DISTRIBUTIONSlcsh:QC770-798High Energy Physics::ExperimentLHCHADRON-COLLISIONSMATTERRealization (systems)TO-LEADING ORDER
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Global analysis of fragmentation functions for eta mesons

2011

Fragmentation functions for eta mesons are extracted at next-to-leading order accuracy of QCD in a global analysis of data taken in electron-positron annihilation and proton-proton scattering experiments. The obtained parametrization is in good agreement with all data sets analyzed and can be utilized, for instance, in future studies of double-spin asymmetries for single-inclusive eta production. The Lagrange multiplier technique is used to estimate the uncertainties of the fragmentation functions and to assess the role of the different data sets in constraining them.

Nuclear and High Energy PhysicsParticle physicsMesonCiencias FísicasElectron–positron annihilationHadronFOS: Physical sciencesElementary particle//purl.org/becyt/ford/1 [https]symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Fragmentation FunctionsNuclear ExperimentQuantum chromodynamicsPhysicsAnnihilation//purl.org/becyt/ford/1.3 [https]QcdEtaAstronomíaHigh Energy Physics - PhenomenologyLagrange multiplierData analysissymbolsHigh Energy Physics::ExperimentCIENCIAS NATURALES Y EXACTASHadronization
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"Table 45" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The D(pT) distributions in different centrality intervals in PbPb and in pp for 158.49 < pTjet < 199.53 and 0.8 < eta < 1.2.

PB PB --> JETS X5020.0(1/Nj)(dN/dpT)p p --> JETS Xjet fragmentation functions
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"Table 57" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The D(pT) distributions in different centrality intervals in PbPb and in pp for 199.53 < pTjet < 251.19 and 0.3 < eta < 0.8.

PB PB --> JETS X5020.0(1/Nj)(dN/dpT)p p --> JETS Xjet fragmentation functions
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"Table 81" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2019

The D(pT) distributions in different centrality intervals in PbPb and in pp for 251.19 < pTjet < 316.22 and 1.2 < eta < 2.1.

PB PB --> JETS X5020.0(1/Nj)(dN/dpT)p p --> JETS Xjet fragmentation functions
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"Table 5" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The D(pT) distributions in different centrality intervals in PbPb and in pp for 158.49 < pTjet < 199.53 and 0.0 < eta < 0.3.

PB PB --> JETS X5020.0(1/Nj)(dN/dpT)p p --> JETS Xjet fragmentation functions
researchProduct

"Table 13" of "Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector"

2020

The D(pT) distributions in different centrality intervals in PbPb and in pp for 251.19 < pTjet < 316.22 and 0.0 < eta < 2.1.

PB PB --> JETS X5020.0(1/Nj)(dN/dpT)p p --> JETS Xjet fragmentation functions
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