Title:
Forward J/ψ production in U + U collisions at sNN =193 GeV

dc.contributor.authorA. Adare
dc.contributor.authorC. Aidala
dc.contributor.authorN.N. Ajitanand
dc.contributor.authorY. Akiba
dc.contributor.authorR. Akimoto
dc.contributor.authorJ. Alexander
dc.contributor.authorM. Alfred
dc.contributor.authorK. Aoki
dc.contributor.authorN. Apadula
dc.contributor.authorH. Asano
dc.contributor.authorE.T. Atomssa
dc.contributor.authorT.C. Awes
dc.contributor.authorB. Azmoun
dc.contributor.authorV. Babintsev
dc.contributor.authorM. Bai
dc.contributor.authorX. Bai
dc.contributor.authorN.S. Bandara
dc.contributor.authorB. Bannier
dc.contributor.authorK.N. Barish
dc.contributor.authorS. Bathe
dc.contributor.authorV. Baublis
dc.contributor.authorC. Baumann
dc.contributor.authorS. Baumgart
dc.contributor.authorA. Bazilevsky
dc.contributor.authorM. Beaumier
dc.contributor.authorS. Beckman
dc.contributor.authorR. Belmont
dc.contributor.authorA. Berdnikov
dc.contributor.authorY. Berdnikov
dc.contributor.authorD. Black
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dc.contributor.authorJ.S. Bok
dc.contributor.authorK. Boyle
dc.contributor.authorM.L. Brooks
dc.contributor.authorJ. Bryslawskyj
dc.contributor.authorH. Buesching
dc.contributor.authorV. Bumazhnov
dc.contributor.authorS. Butsyk
dc.contributor.authorS. Campbell
dc.contributor.authorC.-H. Chen
dc.contributor.authorC.Y. Chi
dc.contributor.authorM. Chiu
dc.contributor.authorI.J. Choi
dc.contributor.authorJ.B. Choi
dc.contributor.authorS. Choi
dc.contributor.authorP. Christiansen
dc.contributor.authorT. Chujo
dc.contributor.authorV. Cianciolo
dc.contributor.authorZ. Citron
dc.contributor.authorB.A. Cole
dc.contributor.authorN. Cronin
dc.contributor.authorN. Crossette
dc.contributor.authorM. Csanád
dc.contributor.authorT. Csörgo
dc.contributor.authorT.W. Danley
dc.contributor.authorA. Datta
dc.contributor.authorM.S. Daugherity
dc.contributor.authorG. David
dc.contributor.authorK. Deblasio
dc.contributor.authorK. Dehmelt
dc.contributor.authorA. Denisov
dc.contributor.authorA. Deshpande
dc.contributor.authorE.J. Desmond
dc.contributor.authorL. Ding
dc.contributor.authorA. Dion
dc.contributor.authorP.B. Diss
dc.contributor.authorJ.H. Do
dc.contributor.authorL. D'Orazio
dc.contributor.authorO. Drapier
dc.contributor.authorA. Drees
dc.contributor.authorK.A. Drees
dc.contributor.authorJ.M. Durham
dc.contributor.authorA. Durum
dc.contributor.authorT. Engelmore
dc.contributor.authorA. Enokizono
dc.contributor.authorS. Esumi
dc.contributor.authorK.O. Eyser
dc.contributor.authorB. Fadem
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dc.contributor.authorD.E. Fields
dc.contributor.authorM. Finger
dc.contributor.authorF. Fleuret
dc.contributor.authorS.L. Fokin
dc.contributor.authorJ.E. Frantz
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dc.contributor.authorA.D. Frawley
dc.contributor.authorY. Fukao
dc.contributor.authorT. Fusayasu
dc.contributor.authorK. Gainey
dc.contributor.authorC. Gal
dc.contributor.authorP. Gallus
dc.contributor.authorP. Garg
dc.contributor.authorA. Garishvili
dc.contributor.authorI. Garishvili
dc.contributor.authorH. Ge
dc.contributor.authorF. Giordano
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dc.contributor.authorY. Goto
dc.contributor.authorR. Granier De Cassagnac
dc.contributor.authorN. Grau
dc.contributor.authorS.V. Greene
dc.contributor.authorM. Grosse Perdekamp
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dc.contributor.authorH. Guragain
dc.contributor.authorT. Hachiya
dc.contributor.authorJ.S. Haggerty
dc.contributor.authorK.I. Hahn
dc.contributor.authorH. Hamagaki
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dc.contributor.authorS.Y. Han
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dc.contributor.authorS. Hasegawa
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dc.contributor.authorK. Hashimoto
dc.contributor.authorR. Hayano
dc.contributor.authorX. He
dc.contributor.authorT.K. Hemmick
dc.contributor.authorT. Hester
dc.contributor.authorJ.C. Hill
dc.contributor.authorR.S. Hollis
dc.contributor.authorK. Homma
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dc.contributor.authorN. Hotvedt
dc.contributor.authorJ. Huang
dc.contributor.authorS. Huang
dc.contributor.authorT. Ichihara
dc.contributor.authorY. Ikeda
dc.contributor.authorK. Imai
dc.contributor.authorY. Imazu
dc.contributor.authorM. Inaba
dc.contributor.authorA. Iordanova
dc.contributor.authorD. Isenhower
dc.contributor.authorA. Isinhue
dc.contributor.authorD. Ivanishchev
dc.contributor.authorB.V. Jacak
dc.contributor.authorS.J. Jeon
dc.contributor.authorM. Jezghani
dc.contributor.authorJ. Jia
dc.contributor.authorX. Jiang
dc.contributor.authorB.M. Johnson
dc.contributor.authorK.S. Joo
dc.contributor.authorD. Jouan
dc.contributor.authorD.S. Jumper
dc.contributor.authorJ. Kamin
dc.contributor.authorS. Kanda
dc.contributor.authorB.H. Kang
dc.contributor.authorJ.H. Kang
dc.contributor.authorJ.S. Kang
dc.contributor.authorJ. Kapustinsky
dc.contributor.authorD. Kawall
dc.contributor.authorA.V. Kazantsev
dc.contributor.authorJ.A. Key
dc.contributor.authorV. Khachatryan
dc.contributor.authorP.K. Khandai
dc.contributor.authorA. Khanzadeev
dc.contributor.authorK.M. Kijima
dc.contributor.authorC. Kim
dc.contributor.authorD.J. Kim
dc.contributor.authorE.-J. Kim
dc.contributor.authorG.W. Kim
dc.contributor.authorM. Kim
dc.contributor.authorY.-J. Kim
dc.contributor.authorY.K. Kim
dc.contributor.authorB. Kimelman
dc.contributor.authorE. Kistenev
dc.contributor.authorR. Kitamura
dc.contributor.authorJ. Klatsky
dc.contributor.authorD. Kleinjan
dc.contributor.authorP. Kline
dc.contributor.authorT. Koblesky
dc.contributor.authorM. Kofarago
dc.contributor.authorB. Komkov
dc.contributor.authorJ. Koster
dc.contributor.authorD. Kotchetkov
dc.contributor.authorD. Kotov
dc.contributor.authorF. Krizek
dc.contributor.authorK. Kurita
dc.contributor.authorM. Kurosawa
dc.contributor.authorY. Kwon
dc.contributor.authorR. Lacey
dc.contributor.authorY.S. Lai
dc.contributor.authorJ.G. Lajoie
dc.contributor.authorA. Lebedev
dc.contributor.authorD.M. Lee
dc.contributor.authorG.H. Lee
dc.contributor.authorJ. Lee
dc.contributor.authorK.B. Lee
dc.contributor.authorK.S. Lee
dc.contributor.authorS. Lee
dc.contributor.authorS.H. Lee
dc.contributor.authorM.J. Leitch
dc.contributor.authorM. Leitgab
dc.contributor.authorB. Lewis
dc.contributor.authorX. Li
dc.contributor.authorS.H. Lim
dc.contributor.authorM.X. Liu
dc.contributor.authorD. Lynch
dc.contributor.authorC.F. Maguire
dc.contributor.authorY.I. Makdisi
dc.contributor.authorM. Makek
dc.contributor.authorA. Manion
dc.contributor.authorV.I. Manko
dc.contributor.authorE. Mannel
dc.contributor.authorT. Maruyama
dc.contributor.authorM. McCumber
dc.contributor.authorP.L. McGaughey
dc.contributor.authorD. McGlinchey
dc.contributor.authorC. McKinney
dc.contributor.authorA. Meles
dc.contributor.authorM. Mendoza
dc.contributor.authorB. Meredith
dc.contributor.authorY. Miake
dc.contributor.authorT. Mibe
dc.contributor.authorA.C. Mignerey
dc.contributor.authorA. Milov
dc.contributor.authorD.K. Mishra
dc.contributor.authorJ.T. Mitchell
dc.contributor.authorS. Miyasaka
dc.contributor.authorS. Mizuno
dc.contributor.authorA.K. Mohanty
dc.contributor.authorS. Mohapatra
dc.contributor.authorP. Montuenga
dc.contributor.authorT. Moon
dc.contributor.authorD.P. Morrison
dc.contributor.authorM. Moskowitz
dc.contributor.authorT.V. Moukhanova
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dc.contributor.authorT. Nagae
dc.contributor.authorS. Nagamiya
dc.contributor.authorK. Nagashima
dc.contributor.authorJ.L. Nagle
dc.contributor.authorM.I. Nagy
dc.contributor.authorI. Nakagawa
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dc.contributor.authorY. Nakamiya
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dc.contributor.authorT. Nakamura
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dc.contributor.authorM. Nihashi
dc.contributor.authorT. Niida
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dc.contributor.authorA. Yanovich
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dc.contributor.authorI. Younus
dc.contributor.authorH. Yu
dc.contributor.authorI.E. Yushmanov
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dc.contributor.authorA. Zelenski
dc.contributor.authorS. Zhou
dc.contributor.authorL. Zou
dc.date.accessioned2026-02-07T08:17:56Z
dc.date.issued2016
dc.description.abstractThe invariant yields, dN/dy, for J/ψ production at forward rapidity (1.2<|y|<2.2) in U+U collisions at sNN=193GeV have been measured as a function of collision centrality. The invariant yields and nuclear-modification 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. © 2016 American Physical Society.
dc.identifier.doi10.1103/PhysRevC.93.034903
dc.identifier.issn24699985
dc.identifier.urihttps://doi.org/10.1103/PhysRevC.93.034903
dc.identifier.urihttps://dl.bhu.ac.in/bhuir/handle/123456789/29413
dc.publisherAmerican Physical Society
dc.titleForward J/ψ production in U + U collisions at sNN =193 GeV
dc.typePublication
dspace.entity.typeArticle

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