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Related papers: Heavy Flavor Physics at the sPHENIX Experiment

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Recent results on identified hadrons from the PHENIX experiment in Au+Au collisions at mid-rapidity at $\sqrt{s_{NN}}$ = 200 GeV are presented. The centrality dependence of transverse momentum distributions and particle ratios for…

Nuclear Experiment · Physics 2009-11-07 T. Chujo

Electro-magnetic probes such as dileptons and photons are strong probes to investigate the thermodynamical state of the early stages of collisions since they leave the system unscathed. The PHENIX experiment has measured both photons and…

Nuclear Experiment · Physics 2019-08-13 Takao Sakaguchi

This article is based on my Proceedings for the 47th Course of the International School of Subnuclear Physics on the Most Unexpected at LHC and the Status of High Energy Frontier, Erice, Sicily, Italy, 2009. Results from the PHENIX…

Nuclear Experiment · Physics 2014-06-04 M. J. Tannenbaum

Transverse momentum ($p_\mathrm{T}$) distribution of electrons for $0.3<p_\mathrm{T}<9.0$ GeV/$c$ have been measured in midrapidity ($|\eta|<0.35$) in Au + Au collisions and $p$ + $p$ collisions at $\sqrt{s_{NN}} = 200$ GeV by the…

Nuclear Experiment · Physics 2008-11-26 F. Kajihara

Data on hadron production at high transverse momentum ($p_T>$ 2 GeV/$c$) in p+p, d+Au, and Au+Au collisions at $\sqrt{s_{NN}$ = 200 GeV from the PHENIX experiment at RHIC are reviewed. The single inclusive spectrum of light hadrons produced…

Nuclear Experiment · Physics 2007-05-23 David d'Enterria

In relativistic heavy ion collisions heavy flavor probes are crucial to understand the interactions between partons and the produced hot nuclear matter. Measurements in p+p collisions provide information about how the heavy quarks are…

Nuclear Experiment · Physics 2019-08-13 Anne Sickles

A systematic study of particle production at large transverse momentum with the PHENIX experiment at RHIC is shown. We demonstrate that the suppression of the yield of high p_T hadrons in central Au+Au collisions compared to the scaled p+p…

Nuclear Experiment · Physics 2007-05-23 Christian Klein-Boesing

It is becoming increasingly clear that initial state effects inherent to collisions of nuclei play an important role in the interpretation of data from heavy ion collisions at RHIC and the LHC. Such effects are more apparent in kinematic…

Nuclear Experiment · Physics 2015-10-28 J. Matthew Durham

The momentum distribution of electrons from decays of heavy flavor (charm and beauty) for midrapidity |y| < 0.35 in p+p collisions at sqrt(s) = 200 GeV has been measured by the PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC)…

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

The latest PHENIX results for particle production are presented in this paper. A suppression of the yield of high p_t (transverse momentum) hadrons in central Au+Au collisions is found. In contrast, direct photons are not suppressed in…

Nuclear Experiment · Physics 2019-08-13 M. Csanad

We report on leptonic observables by the PHENIX experiment from data taken during Run II at the Relativistic Heavy Ion Collider (RHIC). We show first results on phi -> K+K-, e+e-, low and intermediate mass dielectron continuum, single…

Nuclear Experiment · Physics 2019-08-14 J. L. Nagle

For over a decade now, the primary purpose of relativistic heavy-ion collisions at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC) has been to study the properties of QCD matter under extreme conditions -high…

Nuclear Experiment · Physics 2016-07-19 Md. Nasim , Roli Esha , Huan Zhong Huang

Quarkonia provide a sensitive probe of the properties of the hot dense medium created in high energy heavy ion collisions. Hard scattering processes result in the production of heavy quark pairs that interact with the collision medium…

Nuclear Experiment · Physics 2019-08-14 Abigail Bickley

Heavy flavor production in hadronic collisions is dominated by gluonic processes and so is a sensitive probe of the gluon structure function in the nucleon and its modification in nuclei. A study of heavy flavor production in p+p and d+Au…

Nuclear Experiment · Physics 2009-11-11 Xiaorong Wang

Quarks of heavy flavors are useful tool to study quark-gluon plasma created in heavy-ion collisions. Due to their high mass and early production time, heavy quarks experience the entire evolution of the system created in these collisions.…

Nuclear Experiment · Physics 2023-01-11 Leszek Kosarzewski

The silicon pixel detector (SPD) of the ALICE experiment in preparation at the Large Hadron Collider (LHC) at CERN is designed to provide the precise vertex reconstruction needed for measuring heavy flavor production in heavy ion collisions…

Nuclear Experiment · Physics 2012-07-07 Jan Conrad

The PHENIX collaboration presents a concept for a major upgrade to the PHENIX detector at the Relativistic Heavy Ion Collider (RHIC). This upgrade, referred to as sPHENIX, brings exciting new capability to the RHIC program by opening new…

Nuclear Experiment · Physics 2012-07-30 A. Adare , C. Aidala , N. N. Ajitanand , Y. Akiba , R. Akimoto , J. Alexander , K. Aoki , N. Apadula , H. Asano , E. T. Atomssa , T. C. Awes , B. Azmoun , V. Babintsev , M. Bai , X. Bai , N. Bandara , B. Bannier , K. N. Barish , O. Baron , B. Bassalleck , S. Bathe , V. Baublis , S. Baumgart , A. Bazilevsky , M. Beaumier , R. Belmont , G. Benjamin , A. Berdnikov , Y. Berdnikov , X. Bing , D. Black , J. Blackburn , D. S. Blau , M. Bobrek , J. Bok , S. Boose , K. Boyle , C. L. Britton , M. L. Brooks , J. Bryslawskyj , V. Bumazhnov , C. Butler , S. Butsyk , S. Campbell , A. Carollo , J. -S. Chai , C. -H. Chen , S. Chernichenko , C. Y. Chi , M. Chiu , I. J. Choi , J. B. Choi , S. Choi , S. Chollet , P. Christiansen , T. Chujo , V. Cianciolo , B. A. Cole , N. Cronin , N. Crossett , L. D'Orazio , S. Dairaku , A. Datta , M. S. Daugherity , G. David , K. DeBlasio , A. Debraine , K. Dehmelt , A. Denisov , A. Deshpande , E. J. Desmond , O. Dietzsch , L. Ding , A. Dion , J. H. Do , M. Donadelli , O. Drapier , A. Drees , K. A. Drees , J. M. Durham , A. Durum , L. Eberle , S. Edwards , Y. V. Efremenko , T. Engelmore , A. Enokizono , S. Esumi , K. O. Eyser , B. Fadem , D. E. Fields , M. Finger , M. Finger , F. Fleuret , S. L. Fokin , J. E. Frantz , A. Franz , A. D. Frawley , Y. Fukao , T. Fusayasu , K. Gainey , C. Gal , P. Garg , A. Garishvili , I. Garishvili , F. Gastaldi , H. Ge , P. Giannotti , F. Giordarno , A. Glenn , X. Gong , M. Gonin , Y. Goto , R. Granier de Cassagnac , N. Grau , S. V. Greene , M. Grosse Perdekamp , Y. Gu , T. Gunji , H. Guragain , J. S. Haggerty , K. I. Hahn , H. Hamagaki , S. Y. Han , J. Hanks , K. Hashimoto , R. Hayano , S. Hayashi , X. He , T. K. Hemmick , T. Hester , J. C. Hill , M. Hoefferkamp , R. S. Hollis , K. Homma , B. Hong , Y. Hori , T. Hoshino , J. Huang , S. Huang , J. R. Hutchins , T. Ichihara , Y. Ikeda , K. Imai , Y. Imazu , J. Imrek , M. Inaba , A. Iordanova , D. Isenhower , A. Isinhue , D. Ivanischev , V. Ivanov , B. V. Jacak , S. J. Jeon , M. Jezghani , J. Jia , X. Jiang , B. M. Johnson , K. S. Joo , D. Jouan , D. S. Jumper , J. Kamin , S. Kanda , B. H. Kang , J. H. Kang , J. S. Kang , J. Kapustinsky , K. Karatsu , D. Kawall , A. V. Kazantsev , H. -J. Kehayias , J. A. Key , V. Khachatryan , P. K. Khandai , A. Khanzadeev , K. M. Kijima , C. Kim , D. H. Kim , D. J. Kim , E. -J. Kim , H. J. Kim , K. -B. Kim , Y. -J. Kim , Y. K. Kim , E. Kistenev , J. Klatsky , D. Kleinjan , P. Kline , T. Koblesky , L. Kochenda , M. Kofarago , Y. Komatsu , B. Komkov , J. Koster , D. Kotchetkov , D. Kotov , P. Kravtsov , F. Krizek , K. Kurita , M. Kuriyama , M. Kurosawa , Y. Kwon , R. Lacey , Y. S. Lai , J. G. Lajoie , A. Lebedev , G. H. Lee , J. Lee , K. B. Lee , K. S. Lee , S. H. Lee , R. Lefferts , M. J. Leitch , M. A. L. Leite , M. Leitgab , B. Lewis , X. Li , S. H. Lim , A. Lipski , M. X. Liu , B. Love , D. Lynch , M. Lynch , C. F. Maguire , Y. I. Makdisi , M. Makek , A. Manion , V. I. Manko , E. Mannel , T. Maruyama , S. Masumoto , M. McCumber , P. L. McGaughey , D. McGlinchey , R. McKay , C. McKinney , A. Meles , M. Mendoza , R. Menegasso , B. Meredith , Y. Miake , T. Mibe , A. C. Mignerey , A. Milov , D. K. Mishra , J. T. Mitchell , S. Miyasaka , S. Mizuno , A. K. Mohanty , D. P. Morrison , M. Moskowitz , S. Motschwiller , T. V. Moukhanova , T. Murakami , J. Murata , A. Mwai , T. Nagae , S. Nagamiya , J. L. Nagle , M. I. Nagy , I. Nakagawa , Y. Nakamiya , K. R. Nakamura , T. Nakamura , K. Nakano , C. Nattrass , A. Nederlof , P. K. Netrakanti , M. Nihashi , T. Niida , K. Ninomiya , D. Northacker , R. Nouicer , T. Novak , N. Novitzky , A. Nukariya , A. S. Nyanin , E. O'Brien , C. A. Ogilvie , H. Oide , K. Okada , A. Oskarsson , K. Ozawa , R. Pak , C. Pancake , V. Pantuev , V. Papavassiliou , I. H. Park , S. Park , S. K. Park , S. F. Pate , L. Patel , J. -C. Peng , D. Perepelitsa , G. D. N. Perera , D. Yu. Peressounko , J. Perry , R. Petti , C. Pinkenburg , R. P. Pisani , J. Popule , M. L. Purschke , H. Qu , S. Radhakrishnan , J. Rak , I. Ravinovich , K. F. Read , R. Reynolds , V. Riabov , Y. Riabov , E. Richardson , N. Riveli , D. Roach , S. D. Rolnick , M. Rosati , E. Roschin , M. S. Ryu , A. Safonov , B. Sahlmueller , N. Saito , T. Sakaguchi , H. Sako , V. Samsonov , M. Sano , M. Sarsour , S. Sato , S. Sawada , B. Schaefer , K. Sedgwick , J. Seele , R. Seidl , Y. Sekiguchi , A. Sen , R. Seto , P. Sett , E. Shafto , D. Sharma , A. Shaver , I. Shein , T. -A. Shibata , K. Shigaki , M. Shimomura , K. Shoji , P. Shukla , P. Sicho , A. Sickles , C. L. Silva , D. Silvermyr , B. K. Singh , C. P. Singh , V. Singh , F. W. Sippach , M. Skolnik , S. Solano , A. Soldatov , R. A. Soltz , W. E. Sondheim , S. P. Sorensen , M. Soumya , I. V. Sourikova , P. K. Srivastava , P. W. Stankus , P. Steinberg , E. Stenlund , M. Stepanov , A. Ster , L. Stevens , S. P. Stoll , M. R. Stone , T. Sugitate , A. Sukhanov , J. Sun , J. Sziklai , E. M. Takagui , A. Takahara , A. Taketani , Y. Tanaka , K. Tanida , M. J. Tannenbaum , S. Tarafdar , A. Taranenko , A. Tate , E. Tennant , E. Thorsland , A. Timilsina , T. Todoroki , H. Torii , R. Towell , R. S. Towell , V. Trofimov , I. Tserruya , T. Tsuji , A. Tullo , H. W. van Hecke , M. Vargyas , E. Vazquez-Zambrano , A. Veicht , J. Velkovska , M. Virius , V. Vrba , E. Vznuzdaev , X. R. Wang , D. Watanabe , K. Watanabe , Y. Watanabe , Y. S. Watanabe , T. S. Watson , F. Wei , R. Wei , S. Whitaker , D. Winter , S. Wolin , C. L. Woody , M. Wysocki , Y. L. Yamaguchi , R. Yang , A. Yanovich , S. Yokkaichi , I. Yoon , M. Young , I. Younus , I. E. Yushmanov , W. A. Zajc , E. Zarndt , A. Zelenski , L. Zhang , S. Zhou , C. Zumberge

The PHENIX experiment at RHIC measured K0S, eta and omega-meson production at high pT in p+p, d+Au and Au+Au collisions at sqrt(s_NN)=200 GeV. Measurements performed in different hadronic decay channels give consistent results. This paper…

Nuclear Experiment · Physics 2007-07-10 Alexander Milov

Anisotropic flow measurements have demonstrated development of partonic collectivity in $200\mathrm{GeV}$ Au+Au collisions at RHIC. To understand the partonic EOS, thermalization must be addressed. Collective motion of heavy-flavor (c,b)…

Nuclear Experiment · Physics 2019-08-13 Jan Kapitan

Most recent PHENIX results on electromagnetic probes are presented including first preliminary results obtained with the Hadron Blind Detector (HBD) on e+e- invariant mass spectra from Au+Au collisions at sqrt(s_NN) = 200 GeV.

Nuclear Experiment · Physics 2019-08-13 Itzhak Tserruya
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