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dc.contributor.author김용균-
dc.date.accessioned2017-11-08T01:38:32Z-
dc.date.available2017-11-08T01:38:32Z-
dc.date.issued2016-01-
dc.identifier.citationPHYSICAL REVIEW C, v. 93, NO 1, Article number 014904, Page. 1-34en_US
dc.identifier.issn2469-9985-
dc.identifier.issn2469-9993-
dc.identifier.urihttps://journals.aps.org/prc/abstract/10.1103/PhysRevC.93.014904-
dc.identifier.urihttp://hdl.handle.net/20.500.11754/30568-
dc.description.abstractWe present measurements of e(+)e-production at midrapidity in Au + Au collisions at root s(NN) = 200 GeV. The invariant yield is studied within the PHENIX detector acceptance over a wide range of mass (m(ee) ˂ 5 GeV/c(2)) and pair transverse momentum (p(T) ˂ 5 GeV/c) for minimum bias and for five centrality classes. The e(+)e(-) yield is compared to the expectations from known sources. In the low-mass region (m(ee) = 0.30-0.76 GeV/c(2)) there is an enhancement that increases with centrality and is distributed over the entire pair p(T) range measured. It is significantly smaller than previously reported by the PHENIX experiment and amounts to 2.3 +/- 0.4(stat) +/- 0.4(syst) +/- 0.2(model) or to 1.7 +/- 0.3(stat) +/- 0.3(syst) +/- 0.2(model) for minimum bias collisions when the open heavy-flavor contribution is calculated with PYTHIA or MC@NLO, respectively. The inclusive mass and p(T) distributions, as well as the centrality dependence, are well reproduced by model calculations where the enhancement mainly originates from the melting of the rho meson resonance as the system approaches chiral symmetry restoration. In the intermediate-mass region (m(ee) = 1.2-2.8 GeV/c(2)), the data hint at a significant contribution in addition to the yield from the semileptonic decays of heavy-flavor mesons.en_US
dc.description.sponsorshipWe thank the staff of the Collider-Accelerator and Physics Departments at Brookhaven National Laboratory and the staff of the other PHENIX participating institutions for their vital contributions. We also thank R. Rapp for providing us the results of his model calculations and for helpful discussions. We acknowledge support from the Office of Nuclear Physics in the Office of Science of the Department of Energy, the National Science Foundation, Abilene Christian University Research Council, Research Foundation of SUNY, and Dean of the College of Arts and Sciences, Vanderbilt University (USA); Ministry of Education, Culture, Sports, Science, and Technology and the Japan Society for the Promotion of Science (Japan); Conselho Nacional de Desenvolvimento Cientifico e Tecnologico and Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (Brazil); Natural Science Foundation of China (People's Republic of China); Croatian Science Foundation and Ministry of Science, Education, and Sports (Croatia); Ministry of Education, Youth and Sports (Czech Republic); Centre National de la Recherche Scientifique, Commissariat a l'Energie Atomique, and Institut National de Physique Nucleaire et de Physique des Particules (France), Bundesministerium fur Bildung und Forschung, Deutscher Akademischer Austausch Dienst, and Alexander von Humboldt Stiftung (Germany); National Science Fund, OTKA, Karoly Robert University College, and the Ch. Simonyi Fund (Hungary); Department of Atomic Energy and Department of Science and Technology (India); Israel Science Foundation (Israel), Basic Science Research Program through NRF of the Ministry of Education (Korea); Physics Department, Lahore University of Management Sciences (Pakistan); Ministry of Education and Science, Russian Academy of Sciences, Federal Agency of Atomic Energy (Russia); VR and Wallenberg Foundation (Sweden); the U.S. Civilian Research and Development Foundation for the Independent States of the Former Soviet Union, the Hungarian American Enterprise Scholarship Fund, and the US-Israel Binational Science Foundation.en_US
dc.language.isoenen_US
dc.publisherAMER PHYSICAL SOCen_US
dc.subjectSUPER-PROTON SYNCHROTRONen_US
dc.subjectHADRON BLIND DETECTORen_US
dc.subjectLOW-MASS DILEPTONSen_US
dc.subjectPHENIX EXPERIMENTen_US
dc.subjectCHIRAL RESTORATIONen_US
dc.subjectCERN-SPSen_US
dc.subjectCONSTRUCTIONen_US
dc.subjectPERFORMANCEen_US
dc.subjectPAIRSen_US
dc.titleDielectron production in Au plus Au collisions at root s(NN)=200 GeVen_US
dc.typeArticleen_US
dc.relation.no1-
dc.relation.volume93-
dc.identifier.doi10.1103/PhysRevC.93.014904-
dc.relation.page1-34-
dc.relation.journalPHYSICAL REVIEW C-
dc.contributor.googleauthorAdare, A.-
dc.contributor.googleauthorAidala, C.-
dc.contributor.googleauthorAjitanand, N. N.-
dc.contributor.googleauthorAkiba, Y.-
dc.contributor.googleauthorAkimoto, R.-
dc.contributor.googleauthorAlexander, J.-
dc.contributor.googleauthorAlfred, M.-
dc.contributor.googleauthorAl-Ta'ani, H.-
dc.contributor.googleauthorAngerami, A.-
dc.contributor.googleauthorKim, Y. K.-
dc.relation.code2016000902-
dc.sector.campusS-
dc.sector.daehakCOLLEGE OF ENGINEERING[S]-
dc.sector.departmentDEPARTMENT OF NUCLEAR ENGINEERING-
dc.identifier.pidykkim4-


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