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sPHENIX is a high energy nuclear physics experiment under construction at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory (BNL). The primary physics goals of sPHENIX are to study the quark-gluon-plasma, as well as the…

The STAR experiment at the Relativistic Heavy Ion Collider RHIC studies the new state of matter produced in relativistic heavy ion collisions and the spin structure of the nucleon in collisions of polarized protons. In order to improve the…

Instrumentation and Detectors · Physics 2019-08-14 Frank Simon

There are several indications that an opaque partonic medium is created in energetic Au+Au collisions \sqrt{s} ~ 100 GeV/nucleon at the Relativistic Heavy Ion Collider (RHIC). At the extreme densities of ~ 10-100 times normal nuclear…

Nuclear Theory · Physics 2011-09-13 Denes Molnar

A study of heavy flavor production in different collision systems in various kinematic regions presents an opportunity to probe cold nuclear medium and hot dense matter effects. Results from the PHENIX experiment on $J/\psi$ and open charm…

Nuclear Experiment · Physics 2010-12-13 Xiaorong Wang

Measurements of J/$\psi$ production by the PHENIX experiment in p+p, d+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV are reviewed. The results show a suppression beyond what can be explained by cold nuclear matter effects in the…

Nuclear Experiment · Physics 2019-08-13 Ermias T. Atomssa

The $v_{2}$ and $v_{4}$ of pions, kaons and protons have been measured by PHENIX in 200 GeV Au+Au collisions up to $p_{T}$$\sim$6 GeV/c and 4 GeV/c, respectively. The $v_{4}$ of all these identified particles have been found to scale with…

Nuclear Experiment · Physics 2019-08-13 S. Huang

High-energy collisions of heavy ions provide a means to study QCD in a regime of high parton density, and may provide insight into its phase structure. Results from the four experiments at RHIC (BRAHMS, PHENIX, PHOBOS and STAR) are…

Nuclear Experiment · Physics 2009-09-29 Peter Steinberg

The suppression of hadrons with large transverse momentum ($p_{\rm T}$) in central Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 200 GeV compared to a binary scaled p+p reference is one of the major discoveries at RHIC. To understand the nature…

Nuclear Experiment · Physics 2008-03-18 PHENIX Collaboration , Christian Klein-Boesing

The pseudorapidity distribution of charged hadrons produced in Au+Au collisions at a center-of-mass energy of $\sqrt{s_\mathrm{NN}} = 200$ GeV is measured using data collected by the sPHENIX detector. Charged hadron yields are extracted by…

Nuclear Experiment · Physics 2025-09-03 sPHENIX Collaboration , M. I. Abdulhamid , U. Acharya , E. R. Adams , G. Adawi , C. A. Aidala , Y. Akiba , M. Alfred , S. Ali , A. Alsayegh , S. Altaf , H. Amedi , D. M. Anderson , V. V. Andrieux , A. Angerami , N. Applegate , H. Aso , S. Aune , B. Azmoun , V. R. Bailey , D. Baranyai , S. Bathe , A. Bazilevsky , S. Bela , R. Belmont , J. Bennett , J. C. Bernauer , J. Bertaux , R. Bi , A. Bonenfant , S. Boose , C. Borchers , H. Bossi , R. Botsford , R. Boucher , A. Brahma , J. W. Bryan , D. Cacace , I. Cali , M. Chamizo-Llatas , S. B. Chauhan , A. Chen , D. Chen , J. Chen , K. Chen , K. Y. Chen , K. Y. Cheng , C. -Y. Chi , M. Chiu , J. Clement , E. W. Cline , M. Connors , E. Cook , R. Corliss , Y. Corrales Morales , E. Croft , N. d'Hose , A. Dabas , D. Dacosta , M. Daradkeh , S. J. Das , A. P. Dash , G. David , C. T. Dean , K. Dehmelt , X. Dong , A. Drees , J. M. Durham , A. Enokizono , H. Enyo , J. Escobar Cepero , R. Esha , B. Fadem , R. Feder , K. Finnelli , D. Firak , A. Francisco , J. Frantz , A. Frawley , K. Fujiki , M. Fujiwara , B. Garcia , P. Garg , G. Garmire , E. Gentry , Y. Go , C. Goblin , W. Goodman , Y. Goto , A. Grabas , O. Grachov , J. Granato , N. Grau , S. V. Greene , S. K. Grossberndt , R. Guidolini-Cecato , T. Hachiya , J. S. Haggerty , R. Hamilton , J. Hammond , D. A. Hangal , S. Hasegawa , M. Hata , W. He , X. He , T. Hemmick , A. Hodges , M. E. Hoffmann , A. Holt , B. Hong , M. Housenga , S. Howell , Y. Hu , H. Z. Huang , J. Huang , T. C. Huang , D. A. Huffman , C. Hughes , J. Hwang , T. Ichino , M. Ikemoto , D. Imagawa , H. Imai , D. Jah , J. James , H. -R. Jheng , Y. Ji , Z. Ji , H. Jiang , M. Kano , L. Kasper , T. Kato , Y. Kawashima , M. S. Khan , T. Kikuchi , J. Kim , B. Kimelman , H. T. Klest , A. G. Knospe , M. B. Knuesel , H. S. Ko , J. Kuczewski , N. Kumar , R. Kunnawalkam Elayavalli , C. M. Kuo , J. Kvapil , Y. Kwon , J. Lajoie , J. D. Lang , A. Lebedev , S. Lee , L. Legnosky , S. Li , X. Li , T. Lian , S. Liechty , S. Lim , D. Lis , M. X. Liu , W. J. Llope , D. A. Loomis , R. -S. Lu , L. Ma , W. Ma , V. Mahaut , T. Majoros , I. Mandjavidze , E. Mannel , C. Markert , T. R. Marshall , C. Martin , H. Masuda , G. Mattson , M. Mazeikis , C. McGinn , E. McLaughlin , J. Mead , Y. Mei , T. Mengel , M. Meskowitz , J. Mills , A. Milov , C. Mironov , G. Mitsuka , N. Morimoto , D. Morrison , L. W. Mwibanda , C. -J. Naïm , J. L. Nagle , I. Nakagawa , Y. Nakamura , G. Nakano , A. Narde , C. E. Nattrass , D. Neff , S. Nelson , D. Nemoto , P. A. Nieto-Marín , R. Nouicer , G. Nukazuka , E. O'Brien , G. Odyniec , S. Oh , V. A. Okorokov , A. C. Oliveira da Silva , J. D. Osborn , G. J. Ottino , Y. C. Ou , J. Ouellette , D. Padrazo , T. Pani , J. Park , A. Patton , H. Pereira Da Costa , D. V. Perepelitsa , M. Peters , S. Ping , C. Pinkenburg , R. Pisani , C. Platte , C. Pontieri , T. Protzman , M. L. Purschke , J. Putschke , R. J. Reed , L. Reeves , S. Regmi , E. Renner , D. Richford , C. Riedl , T. Rinn , C. Roland , G. Roland , A. Romero Hernandez , M. Rosati , D. Roy , A. Saed , T. Sakaguchi , H. Sako , S. Salur , J. Sandhu , M. Sarsour , S. Sato , B. Sayki , B. Schaefer , J. Schambach , R. Seidl , B. D. Seidlitz , Y. Sekiguchi , M. Shahid , D. M. Shangase , Z. Shi , C. W. Shih , K. Shiina , M. Shimomura , R. Shishikura , E. Shulga , A. Sickles , D. Silvermyr , R. A. Soltz , W. Sondheim , I. Sourikova , P. Steinberg , D. Stewart , S. Stoll , Y. Sugiyama , O. Suranyi , W. -C. Tang , S. Tarafdar , E. Thorsland , T. Todoroki , L. S. Tsai , H. Tsujibata , M. Tsuruta , J. Tutterow , E. Tuttle , B. Ujvari , E. N. Umaka , M. Vandenbroucke , J. Vasquez , J. Velkovska , V. Verkest , A. Vijayakumar , X. Wang , Y. Wang , Z. Wang , I. S. Ward , M. Watanabe , J. Webb , A. Wehe , A. Wils , V. Wolfe , C. Woody , W. Xie , Y. Yamaguchi , Z. Ye , K. Yip , Z. You , G. Young , C. -J. Yu , X. Yu , X. Yu , W. A. Zajc , V. Zakharov , J. Zhang , C. Zimmerli

The first results from Au-Au collisions at $\sqrt{s_{NN}}$=130 GeV obtained with the PHENIX detector in the Year 2000 run at RHIC are presented. The mid-rapidity charged particle multiplicity and transverse energy per participating nucleon…

Nuclear Experiment · Physics 2019-08-14 A. Bazilevsky

Hadron collisions at the LHC offer a unique opportunity to study strong interactions. The exciting data collected by the four RHIC experiments suggest that in heavy-ion collisions at sqrt(s_NN) = 200 GeV, an equilibrated, strongly-coupled…

Nuclear Experiment · Physics 2007-05-23 Christof Roland

The anisotropy parameter v_2, the second harmonic of the azimuthal particles distribution, has been measured with the PHENIX detector in Au+Au collisions at sqrt(s_NN) = 200 GeV for identified and inclusive charged particles at central…

Nuclear Experiment · Physics 2008-11-26 PHENIX Collaboration , S. S. Adler

Transverse momentum (p_T) spectra of neutral pions and charged hadrons measured in Au+Au and d+Au collisions at sqrt{s_NN}=200 GeV by the PHENIX experiment at RHIC are compared to p+p reference spectra at the same sqrt{s_NN}. In central…

Nuclear Experiment · Physics 2019-08-14 Klaus Reygers

It has been established that "hard probes", observables involving high-momentum transfer, provide useful tools for studying the hot, dense medium created in nucleus-nucleus collisions at RHIC. The nuclear modification factor, azimuthal…

Nuclear Experiment · Physics 2009-11-11 David Winter

Recent results indicate that the J/psi suppression pattern differs with rapidity showing a larger suppression at forward rapidity. J/psi suppression mechanisms based on energy density (such as color screening, interaction with co-movers,…

Nuclear Experiment · Physics 2019-08-13 Catherine Silvestre

The Intermediate Silicon Tracker (INTT), a two-layer barrel silicon strip tracker, is a key component of the tracking system for sPHENIX at the Relativistic Heavy Ion Collider (RHIC) at Brookhaven National Laboratory. The INTT is designed…

The intermediate $p_T$ region (2 - 5 GeV/$c$) in central Au+Au collisions at RHIC has a rich physics content. The (anti)proton to pion ratio at the intermediate $p_T$ gives us a powerful tool to investigate the bulk properties of the hot…

Nuclear Experiment · Physics 2019-08-14 T. Chujo

Photons are emitted at all stages of relativistic heavy-ion collisions and do not interact with the medium strongly. With access to the versatility of RHIC, measurements of low momentum direct photons are made possible across different…

Nuclear Experiment · Physics 2023-09-12 Roli Esha

PHENIX measurements of high transverse momentum ($p_T$) identified hadrons in $d$+Au and Au+Au collisions are presented. The nuclear modification factors ($R_{d{\rm A}}$ and $R_{\rm AA}$) for $\pi^0$ and $\eta$ are found to be very…

Nuclear Experiment · Physics 2019-08-13 Takao Sakaguchi

Au+Au, $\sqrt{s} = 200$ A GeV measurements at RHIC, obtained with the PHENIX, STAR, PHOBOS and BRAHMS detectors, have all indicated a suppression of production, relative to an appropriately normalized NN level. For central collisions and…

Nuclear Theory · Physics 2007-05-23 D. E. Kahana , S. H. Kahana