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Related papers: Heavy Flavor Physics at the sPHENIX Experiment

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Measurements of inclusive spectra of hadrons at large transverse momentum over a broad range of energy in different collision systems have been performed with the PHENIX experiment at RHIC. The data allow to study the energy and system size…

Nuclear Experiment · Physics 2008-11-26 B. Sahlmueller

PHENIX measures leptons at mid and forward rapidities and extracts leptons resulting from semi-leptonic decays of heavy quarks. We present PHENIX results related to heavy quark production, specifically the invariant cross section of the…

Nuclear Experiment · Physics 2009-11-11 Y. Kwon

Measurements from the RHIC experiments show strong suppression of high-pT hadrons in central Au+Au collisions. The PHENIX experiment has observed strong suppression of $\pi^0$ and charged hadron yields in central Au+Au collisions for pT > 5…

Nuclear Experiment · Physics 2009-11-11 Tadaaki Isobe

The PHENIX experiment uses semileptonic decay channels to measure open and closed heavy flavor cross sections across the rapidity range $-2.2 < y < 2.4$. High luminosity data are now available for p+p, d+Au, Cu+Cu and Au+Au collisions at…

Nuclear Experiment · Physics 2019-08-21 A. D. Frawley

The PHENIX experiment has measured {\piz}s in Au+Au collisions at sqrt(s_{NN}) = 200 GeV, with good statistics for transverse momentum, pT, up to 20 GeV/c. A fivefold suppression is found, which is essentially constant for 5<pT<20 GeV/c.…

Nuclear Experiment · Physics 2019-08-13 D. Winter

Measurements of light hadron production in ultrarelativistic nuclear collisions provide essential insight into final-state effects arising from both hot and cold nuclear matter. They probe collective behavior, hadronization via…

Nuclear Experiment · Physics 2026-04-21 Murad Sarsour

Quarkonium is an ideal probe to explore the properties of quantum chromodynamics (QCD). Unlike Large Hadron Collider (LHC) measurements, quarkonium production at the Relativistic Heavy Ion Collider (RHIC) has different production…

Nuclear Experiment · Physics 2024-10-15 Xuan Li

Jet related observables have been some of the most powerful and exciting probes for understanding the matter produced in ultra-relativistic heavy ion collisions. Full jet reconstruction was begun at RHIC, and the LHC experiments have shown…

Nuclear Experiment · Physics 2019-08-13 Anne M. Sickles

The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has measured electrons from heavy flavor (charm and bottom) decays for 0.3 < p_T < 9 GeV/c at midrapidity (|y| < 0.35) in Au+Au collisions at sqrt(s_NN) = 200 GeV. The…

Nuclear Experiment · Physics 2008-11-26 PHENIX Collaboration , A. Adare

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

Forward hadron measurements in p(d)+A provide a signal to study nuclear shadowing, initial state energy loss and/or gluon saturation effects as a function of rapidity, centrality and energy. High $p_T$ identified $\pi^{0}$ measurements are…

Nuclear Experiment · Physics 2019-02-20 Jason Bryslawskyj

The PHENIX experiment at the Relativistic Heavy Ion Collider has measured single electrons at midrapidity and single muons at forward and backward rapidities (1.2<|y|< 2.2) for p+p and d+Au collisions at sqrt(sNN)=200 GeV. The inclusive…

Nuclear Experiment · Physics 2009-09-29 Y. Kwon

The sPHENIX detector to be installed at RHIC in 2022 is designed to precisely measure jets, jet correlations, and dilepton pairs in heavy-ion collisions. With these measurements in mind, sPHENIX will employ a compact TPC covering 20cm < r <…

Instrumentation and Detectors · Physics 2022-12-13 Henry T. Klest

During the past several years, experiments at RHIC have established that a dense partonic medium is produced in Au+Au collisions at sqrt(s)=200 GeV. Subsequently, a primary goal of analysis has been to understand and characterize the…

Nuclear Experiment · Physics 2019-08-13 David Winter

This paper reports measurements of the transverse energy per unit pseudorapidity ($dE_{T}/d\eta$) produced in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV, performed with the sPHENIX detector at the Relativistic Heavy Ion Collider (RHIC).…

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 production of the low-mass dielectrons is considered to be a powerful tool to study the properties of the hot and dense matter created in the ultra-relativistic heavy-ion collisions. We present the preliminary results on the first…

Nuclear Experiment · Physics 2008-11-26 Alexander Kozlov

The PHENIX and STAR Collaborations at the Relativistic Heavy-Ion Collider and ALICE, CMS, ATLAS and LHCb Collaborations at the Large Hadron Collider have measured the production of charmonium and bottonium states as well as open heavy…

Nuclear Experiment · Physics 2018-11-13 Andrea Dubla

The first measurement of the dielectron continuum at RHIC energies was performed by the PHENIX experiment for Au+Au collisions at sqrt(s_{NN}) = 200 GeV. Mass spectra for different centralities are presented and compared with the…

Nuclear Experiment · Physics 2019-08-14 Alberica Toia

Electromagnetic probes are ideally suited to investigate hot and dense matter produced in high energy heavy ion collisions. They do not undergo strong interactions and thus probe the time evolution of the collision. The dielectron continuum…

Nuclear Experiment · Physics 2015-06-26 Alberica Toia