dc.contributor.author | PHENIX Collaboration | |
dc.date.accessioned | 2016-06-03T10:05:18Z | |
dc.date.available | 2016-06-03T10:05:18Z | |
dc.date.issued | 2016 | |
dc.identifier.citation | PHENIX Collaboration. (2016). Forward J/ψ production in U+U collisions at √sNN = 193 GeV. <i>Physical Review C</i>, <i>93</i>(3), Article 034903. <a href="https://doi.org/10.1103/PhysRevC.93.034903" target="_blank">https://doi.org/10.1103/PhysRevC.93.034903</a> | |
dc.identifier.other | CONVID_25619107 | |
dc.identifier.uri | https://jyx.jyu.fi/handle/123456789/50080 | |
dc.description.abstract | The invariant yields, dN/dy, for J/ψ production at forward rapidity (1.2 < |y| < 2.2) in U + U collisions
at √sNN = 193 GeV have been measured as a function of collision centrality. The invariant yields and nuclearmodification
factor RAA are presented and compared with those from Au + Au collisions in the same rapidity
range. Additionally, the direct ratio of the invariant yields from U + U and Au + Au collisions within the same
centrality class is presented, and used to investigate the role of cc¯ coalescence. Two different parametrizations
of the deformed Woods-Saxon distribution were used in Glauber calculations to determine the values of the
number of nucleon-nucleon collisions in each centrality class, Ncoll, and these were found to give significantly
different Ncoll values. Results using Ncoll values from both deformed Woods-Saxon distributions are presented.
The measured ratios show that the J/ψ suppression, relative to binary collision scaling, is similar in U + U
and Au + Au for peripheral and midcentral collisions, but that J/ψ show less suppression for the most central
U + U collisions. The results are consistent with a picture in which, for central collisions, increase in the J/ψ
yield due to cc¯ coalescence becomes more important than the decrease in yield due to increased energy density.
For midcentral collisions, the conclusions about the balance between cc¯ coalescence and suppression depend on
which deformed Woods-Saxon distribution is used to determine Ncoll. | |
dc.language.iso | eng | |
dc.publisher | American Physical Society | |
dc.relation.ispartofseries | Physical Review C | |
dc.subject.other | U+U collisions | |
dc.subject.other | J/psi mesons | |
dc.title | Forward J/ψ production in U+U collisions at √sNN = 193 GeV | |
dc.type | research article | |
dc.identifier.urn | URN:NBN:fi:jyu-201606032840 | |
dc.contributor.laitos | Fysiikan laitos | fi |
dc.contributor.laitos | Department of Physics | en |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | |
dc.date.updated | 2016-06-03T09:15:04Z | |
dc.type.coar | http://purl.org/coar/resource_type/c_2df8fbb1 | |
dc.description.reviewstatus | peerReviewed | |
dc.relation.issn | 2469-9985 | |
dc.relation.numberinseries | 3 | |
dc.relation.volume | 93 | |
dc.type.version | publishedVersion | |
dc.rights.copyright | © 2016 American Physical Society. Published in this repository with the kind permission of the publisher. | |
dc.rights.accesslevel | openAccess | fi |
dc.type.publication | article | |
dc.relation.doi | 10.1103/PhysRevC.93.034903 | |
dc.type.okm | A1 | |