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dc.contributor.authorPHENIX Collaboration
dc.date.accessioned2024-04-30T10:52:22Z
dc.date.available2024-04-30T10:52:22Z
dc.date.issued2024
dc.identifier.citationPHENIX Collaboration. (2024). Charm- and bottom-quark production in Au+Au collisions at √sNN = 200 GeV. <i>Physical Review C</i>, <i>109</i>(4), Article 044907. <a href="https://doi.org/10.1103/PhysRevC.109.044907" target="_blank">https://doi.org/10.1103/PhysRevC.109.044907</a>
dc.identifier.otherCONVID_213405812
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/94598
dc.description.abstractThe invariant yield of electrons from open-heavy-flavor decays for 1<8 GeV/c at midrapidity |y|<0.35 in Au+Au collisions at √sNN = 200 GeV has been measured by the PHENIX experiment at the BNL Relativistic Heavy Ion Collider. A displaced-vertex analysis with the PHENIX silicon-vertex detector enables extraction of the fraction of charm and bottom hadron decays and unfolding of the invariant yield of parent charm and bottom hadrons. The nuclear-modification factors RAA for electrons from charm and bottom hadron decays and heavy-flavor hadrons show both a centrality and a quark-mass dependence, indicating suppression in the quark-gluon plasma produced in these collisions that is medium sized and quark-mass dependent.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review C
dc.rightsIn Copyright
dc.titleCharm- and bottom-quark production in Au+Au collisions at √sNN = 200 GeV
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202404303225
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2469-9985
dc.relation.numberinseries4
dc.relation.volume109
dc.type.versionpublishedVersion
dc.rights.copyright© 2024 American Physical Society
dc.rights.accesslevelopenAccessfi
dc.subject.ysohiukkasfysiikka
dc.subject.ysokvarkki-gluoniplasma
dc.subject.ysokvarkit
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p38826
jyx.subject.urihttp://www.yso.fi/onto/yso/p19627
dc.rights.urlhttp://rightsstatements.org/page/InC/1.0/?language=en
dc.relation.doi10.1103/PhysRevC.109.044907
jyx.fundinginformationWe 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), Natural Science Foundation of China (People's Republic of China), Croatian Science Foundation and Ministry of Science and Education (Croatia), Ministry of Education, Youth and Sports (Czech Republic), Centre National de la Recherche Scientifique, Commissariat à l'Énergie Atomique, and Institut National de Physique Nucléaire et de Physique des Particules (France), J. Bolyai Research Scholarship, EFOP, the New National Excellence Program (ÚNKP), NKFIH, and OTKA (Hungary), Department of Atomic Energy and Department of Science and Technology (India), Israel Science Foundation (Israel), Basic Science Research and SRC(CENuM) Programs through NRF funded by the Ministry of Education and the Ministry of Science and ICT (Korea), Ministry of Education and Science, Russian Academy of Sciences, Federal Agency of Atomic Energy (Russia), VR and Wallenberg Foundation (Sweden), University of Zambia, the Government of the Republic of Zambia (Zambia), the U.S. Civilian Research and Development Foundation for the Independent States of the Former Soviet Union, the Hungarian American Enterprise Scholarship Fund, the US-Hungarian Fulbright Foundation, and the US-Israel Binational Science Foundation.
dc.type.okmA1


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