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Related papers: Implementation of ACTS into sPHENIX track reconstr…

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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

With the measurement of several observables at SPS energies that demonstrate non-monotonic behavior as a function of centrality and $\sqrt{s_{NN}}$, there is growing interest in pursuing a scan of relativistic heavy ion collisions at low…

Nuclear Experiment · Physics 2007-05-23 J. T. Mitchell

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

The central arm spectrometers for the PHENIX experiment at the Relativistic Heavy Ion Collider have been designed for the optimization of particle identification in relativistic heavy ion collisions. The spectrometers present a challenging…

Nuclear Experiment · Physics 2009-11-07 J. T. Mitchell , PHENIX Collaboration

Cold nuclear matter (CNM) effects provide an important baseline for the interpretation of data in heavy ion collisions. Such effects include nuclear shadowing, Cronin effect, and initial patron energy loss, and it is interesting to study…

Nuclear Experiment · Physics 2019-08-21 Sanghoon Lim

The PHENIX Collaboration has actively pursued a Data and Analysis Preservation program since 2019, the first such dedicated effort at RHIC. A particularly challenging aspect of this endeavor is preservation of complex physics analyses,…

Data Analysis, Statistics and Probability · Physics 2024-08-23 Gabor David , Maxim Potekhin , Dmitri Smirnov

The Relativistic Heavy Ion Collider collides heavy nuclei at ultrarelativistic energies, creating a strongly interacting, partonic medium that is opaque to the passage of high energy quarks and gluons. Direct jet reconstruction applied to…

Nuclear Experiment · Physics 2019-08-13 Yue-Shi Lai

The polarized proton beams at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory provide a unique environment to observe hard scattering between gluons and quarks. The PHENIX experiment has recorded collisions at…

Nuclear Experiment · Physics 2009-05-19 Astrid Morreale

Measurement of heavy quark production is one of the tools used to investigate the matter produced in extremely hot and dense conditions in heavy ion collisions at RHIC. The PHENIX experiment has measured mid-rapidity transverse momentum…

High Energy Physics - Experiment · Physics 2019-08-14 Cesar Luiz Silva

This R\&D project, initiated by the DOE Nuclear Physics AI-Machine Learning initiative in 2022, leverages AI to address data processing challenges in high-energy nuclear experiments (RHIC, LHC, and future EIC). Our focus is on developing a…

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

We describe a start-timing detector for the PHENIX experiment at the relativistic heavy-ion collider RHIC. The role of the detector is to detect a nuclear collision, provide precise time information with an accuracy of 50ps, and determine…

Instrumentation and Detectors · Physics 2009-10-31 K. Ikematsu , Y. Iwata , K. Kaimi , M. Kaneta , T. Kohama , N. Maeda , K. Matsukado , H. Ohnishi , K. Ono , A. Sakaguchi , T. Sugitate , Y. Sumi , Y. Takata , M. Tanabe , A. Yokoro

The J/$\psi$ yields in heavy ion collisions are expected to be a promising probe of deconfined matter, since theoretical models predict that the J/$\psi$ production could be strongly suppressed due to color screening effect in a Quark Gluon…

Nuclear Experiment · Physics 2019-08-14 VN Tram

A sophisticated trigger system, capable of real-time track reconstruction, is used in the ATLAS experiment to select interesting events in the proton-proton collisions at the Large Hadron Collider at CERN. A set of $b$-jet triggers was…

High Energy Physics - Experiment · Physics 2015-06-03 Andrea Coccaro

With an electron-positron collider operating at center-of-mass-energy 2-7 GeV and a peak luminosity above $0.5\times10^{35} cm^{-2} s^{-1}$, the STCF physics program will provide an unique platform for in-depth studies of hadron structure…

High Energy Physics - Experiment · Physics 2023-07-26 Xiaocong Ai , Xingtao Huang , Yi Liu

One of the fundamental goals of the PHENIX experiment is to understand the structure of cold nuclear matter, since this serves as the initial state for heavy-ion collisions. Knowing the initial state is vital for interpreting measurements…

Nuclear Experiment · Physics 2012-10-10 Mickey Chiu

From the wealth of data obtained from the first three years of RHIC operation, the four RHIC experiments, BRAHMS, PHENIX, PHOBOS and STAR, have concluded that a high density partonic matter is formed at central Au+Au collisions at 200 GeV.…

Nuclear Experiment · Physics 2019-08-13 Rachid Nouicer

The properties of jets produced in p+p, d+Au and Au+Au collisions at sqrt{s_NN}=200 GeV are studied using the method of two particle correlations. The trigger particle is assumed to be a leading particle from a high p_T jet while the…

High Energy Physics - Experiment · Physics 2009-11-10 Jan Rak

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

The PHENIX experiment at RHIC has a unique large rapidity coverage ($1.2 < |y| < 2.2$) for heavy flavor studies in heavy-ion collisions. This kinematic region has a smaller particle density and may undergo different nuclear effects before…

Nuclear Experiment · Physics 2024-07-04 Krista Smith