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Nuclear matter effects on J / ψ production in asymmetric Cu + Au collisions at s N N = 200 GeVPion and kaon production in central Pb + Pb collisions at 20 A and 30 A GeV: Evidence for the onset of deconfinementEnhanced J / ψ production in deconfined quark matterEvidence for Statistical Production of J / ψ Mesons in Nuclear Collisions at 158–200 A GeVQCD and strongly coupled gauge theories: challenges and perspectives.J/ψ Elliptic Flow in Pb-Pb Collisions at sqrt[s_{NN}]=5.02 TeV.J/psi suppression in nucleus-nucleus collisions.In-medium effects on charmonium production in heavy-ion collisions.Measurement of an Excess in the Yield of J/ψ at Very Low p_{T} in Pb-Pb Collisions at sqrt[s]_{NN}=2.76 TeV.J/psi production in quark-gluon plasma.Centrality dependence of charm production from a measurement of single electrons in Au+Au collisions at sqrt[s(NN)]=200 GeV.J/ψ elliptic flow in Pb-Pb collisions at √(s(NN))=2.76 TeV.J/ψ suppression at forward rapidity in Pb-Pb collisions at √s(NN) = 2.76 TeV.Cold nuclear matter effects on J/ψ yields as a function of rapidity and nuclear geometry in d+A collisions at sqrt[s(NN)]=200 GeV.Open charm as a probe of preequilibrium dynamics in nuclear collisions.Passage of high-energy partons through a quark-gluon plasma.Charmonium production versus open charm in nuclear collisions.Percolation Approach to Quark-Gluon Plasma and J/ psi Suppression.Challenges in QCD matter physics --The scientific programme of the Compressed Baryonic Matter experiment at FAIRRelative Modification of Prompt ψ(2S) and J/ψ Yields from pp to PbPb Collisions at sqrt[s_{NN}]=5.02 TeVMeasurement of prompt and nonprompt [Formula: see text] production in [Formula: see text] and [Formula: see text] collisions at [Formula: see text]Suppression and azimuthal anisotropy of prompt and nonprompt [Formula: see text] production in PbPb collisions at [Formula: see text][Formula: see text]Measurement of Promptψ(2S)toJ/ψYield Ratios in Pb-Pb andp-pCollisions atsNN=2.76 TeVEvent activity dependence of $ Y $ (nS) production in $ \sqrt{{{s_{NN }}}} $ = 5.02 TeV pPb and $ \sqrt{s} $ = 2.76 TeV pp collisionsObservation of Sequential ϒ Suppression in PbPb CollisionsSuppression of non-prompt J/ψ, prompt J/ψ, and $ \Upsilon $ (1S) in PbPb collisions at $ \sqrt {{{s_{\text{NN}}}}} = 2.76 $ TeVIndications of Suppression of ExcitedΥStates in Pb-Pb Collisions atsNN=2.76 TeVMeasurement of differentialJ/ψproduction cross sections and forward-backward ratios inp + Pbcollisions with the ATLAS detectorCharmonium absorption by nucleonsQuarkonium above deconfinement as an open quantum systemQuarkonia correlators above deconfinementNuclear-modification factor for open-heavy-flavor production at forward rapidity in Cu+Cu collisions atsNN=200GeVDetailed measurement of thee+e−pair continuum inp+pandAu+Aucollisions atsNN=200GeV and implications for direct photon productionMeasurement of single muons at forward rapidity inp+pcollisions ats=200 GeVand implications for charm productionSingle Electrons from Heavy-Flavor Decays inp+pCollisions ats=200 GeVJ∕ψproduction inAu-Aucollisions atsNN=200GeVStudy of ψ(2S) production and cold nuclear matter effects in pPb collisions at s N N = 5 $$ \sqrt{s_{N\;N}}=5 $$ TeVStudy of J/ψ production and cold nuclear matter effects in pPb collisions at $ \sqrt{{{s_{NN }}}} $ = 5 TeVStudy of ϒ $$ \varUpsilon $$ production and cold nuclear matter effects in pPb collisions at s NN $$ \sqrt{s_{NN}} $$ = 5 TeVMeasurement of the relative yields of ψ(2S) to ψ(1S) mesons produced at forward and backward rapidity in p+p , p+Al , p+Au , and He3+Au collisions at sNN=200 GeV
P2860
Q21707745-B82CE1DF-3E19-447F-99B4-6B2F42D2ACB4Q21707762-C384C848-0684-476D-AD63-1E899893AC83Q21708303-E01DCDE1-D1D3-4666-B217-9B0ADB7229CEQ27335625-B06BA95A-E3AF-49FC-BBA0-6315B38F55B4Q42583146-D6CA079B-11AE-4AC7-B2C8-D42987880F83Q49495815-9C5D0A24-49F3-4C23-AC48-9307157D9036Q50111896-337343AC-143F-4294-B934-CCE0F21891E1Q50145323-743BF65E-DC93-40E8-B980-C187A9617D92Q50625553-DFDB5AD3-3DC2-40DA-82B4-CC7A48943FE8Q51923296-D6DD5117-04CD-4476-AE57-D42888D62E31Q52975047-F3D8534C-DFBD-475F-8742-3FB00DE1195FQ53310087-C1376A44-CF6B-4CC7-8B78-9E6BCEBEBA11Q53359562-26DC26B9-321D-4AA8-A12E-AF1D823111ADQ53397376-DEF0A4D3-CCCE-489F-A508-67CEC769C4C9Q54011353-F5860D55-92EE-4ABE-B9DC-5D7FF9CC753FQ54016770-E62EF759-6E11-4E77-9A08-E11CDDAB836DQ54023822-ECF2C1AB-EFCB-436B-852E-1B440E4E48E4Q54104181-5CA10095-15F3-4A62-B652-CCA012BF9E1DQ55950608-4556C447-6F4B-4A3C-B74D-FB39C22CAFE1Q56524927-947CAEB4-5BA6-4CF2-AEF9-E35CBF885388Q56547525-F1683D18-A8C9-4A84-84CE-1E3904B6C871Q56547532-C72690A6-5240-47DA-9291-67D775A4649EQ56628585-03B82335-7B56-4765-ACA9-AEA8DC823838Q56674903-9CC38C40-92BB-431D-A9FC-0E3774AE2598Q56742402-C199FD3C-2CC1-494E-97A5-899D3E9EA8E6Q56743324-22C1AF63-55C7-4E99-BE7B-5A63C31DEE22Q56744023-44F99208-7067-427A-ADEF-B20BC83910B2Q57007833-E7CBC6D6-580D-4334-8A1C-0452DECA9F1CQ57407321-BF2C2FE3-AD51-40F2-9113-AEA7BBA6B065Q57426622-D48AAC66-09EE-472A-94DD-F8FAB75B3547Q57480339-ED192B56-C9EF-4038-897D-B9C570692D1FQ57516000-65242034-E86D-4AF5-8FEB-F725740D45B4Q57516067-48B912EF-6B4D-44D5-8CBC-BA1C96C13A95Q57516100-2652B957-D7FD-4371-B47C-01A608396D40Q57516154-9872894E-A289-4B12-AA4E-2B063DD45163Q57516214-2525EA39-4687-4A89-8517-51384735F818Q57529654-520237F8-EE08-477F-A944-39BA2B36BA6CQ57529925-2A6C2B41-D254-4E5D-A2FE-3AF12219A344Q57530025-114509C9-72FC-422A-A716-E39AF627E7C8Q57545152-F2DC718A-768A-4938-9E31-0076666E7665
P2860
description
im Oktober 1986 veröffentlichter wissenschaftlicher Artikel
@de
wetenschappelijk artikel
@nl
наукова стаття, опублікована в жовтні 1986
@uk
name
J/ψ suppression by quark-gluon plasma formation
@en
J/ψ suppression by quark-gluon plasma formation
@nl
type
label
J/ψ suppression by quark-gluon plasma formation
@en
J/ψ suppression by quark-gluon plasma formation
@nl
prefLabel
J/ψ suppression by quark-gluon plasma formation
@en
J/ψ suppression by quark-gluon plasma formation
@nl
P1433
P1476
J/ψ suppression by quark-gluon plasma formation
@en
P2093
P304
P356
10.1016/0370-2693(86)91404-8
P577
1986-10-01T00:00:00Z