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Related papers: Phi Meson Measurements at RHIC with the PHENIX Det…

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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

Measurements at RHIC have established the creation of a Quark Gluon Plasma (QGP) in most central heavy-ion collisions. An important tool to understand properties of the QGP is study of the spectral shapes of low-mass vector mesons (LVM's),…

High Energy Physics - Experiment · Physics 2019-08-13 Yuji Tsuchimoto

$\phi$ meson measurements provide insight into strangeness production, which is one of the key observables for the hot medium formed in high-energy heavy-ion collisions. ALICE measured $\phi$ production through its decay in muon pairs in…

Nuclear Experiment · Physics 2019-01-18 ALICE Collaboration

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

The measurement of quarkonia production in relativistic heavy ion collisions provides a powerful tool for studying the properties of the hot and dense matter created in these collisions. To be really useful, however, such measurements must…

Nuclear Experiment · Physics 2015-09-14 Alexandre Lebedev

The heavy quarks produced in the early stage of heavy-ion collisions are very effective probes of the dense partonic medium produced at RHIC. PHENIX has the ability to measure heavy quark production through single electrons in the central…

High Energy Physics - Experiment · Physics 2015-06-18 Sanghoon Lim

The PHENIX experiment at RHIC has measured a variety of light neutral mesons ($\pi^{0}$, K$_{S}^{0}$, $\eta$, $\omega$, $\eta^{\prime}$, $\phi$) via multi-particle decay channels over a wide range of transverse momentum. A review of the…

Nuclear Experiment · Physics 2009-03-08 M. Naglis

Recent results on the identified charged-hadron ($\pi^\pm$, $K^\pm$, $p$, $\bar{p}$) production at midrapidity region ($|\eta|<$ 0.35) have been measured by the PHENIX experiment in ${\rm {\it p}+Al}$, ${\rm ^{3}He+Au}$, ${\rm Cu+Au}$…

Nuclear Experiment · Physics 2024-11-22 Rachid Nouicer

The PHENIX experiment reports systematic measurements at the Relativistic Heavy Ion Collider of $\phi$-meson production in asymmetric Cu$+$Au collisions at $\sqrt{s_{_{NN}}}$=200 GeV and in U$+$U collisions at $\sqrt{s_{_{NN}}}$=193 GeV.…

Nuclear Experiment · Physics 2023-01-16 N. J. Abdulameer , U. Acharya , C. Aidala , N. N. Ajitanand , Y. Akiba , R. Akimoto , J. Alexander , M. Alfred , M. Alibordi , K. Aoki , N. Apadula , H. Asano , E. T. Atomssa , T. C. Awes , B. Azmoun , V. Babintsev , M. Bai , X. Bai , B. Bannier , K. N. Barish , S. Bathe , V. Baublis , C. Baumann , S. Baumgart , A. Bazilevsky , M. Beaumier , R. Belmont , A. Berdnikov , Y. Berdnikov , L. Bichon , D. Black , B. Blankenship , D. S. Blau , J. S. Bok , V. Borisov , K. Boyle , M. L. Brooks , J. Bryslawskyj , H. Buesching , V. Bumazhnov , S. Butsyk , S. Campbell , V. Canoa Roman , C. -H. Chen , M. Chiu , C. Y. Chi , I. J. Choi , J. B. Choi , S. Choi , P. Christiansen , T. Chujo , V. Cianciolo , B. A. Cole , M. Connors , R. Corliss , Y. Corrales Morales , N. Cronin , N. Crossette , M. Csanád , T. Csörgő , L. D'Orazio , A. Datta , M. S. Daugherity , G. David , C. T. Dean , K. Dehmelt , A. Denisov , A. Deshpande , E. J. Desmond , L. Ding , V. Doomra , J. H. Do , O. Drapier , A. Drees , K. A. Drees , J. M. Durham , A. Durum , T. Engelmore , A. Enokizono , R. Esha , K. O. Eyser , B. Fadem , W. Fan , D. E. Fields , M. Finger, , M. Finger , D. Firak , D. Fitzgerald , 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 , M. Giles , F. Giordano , A. Glenn , X. Gong , M. Gonin , Y. Goto , R. Granier de Cassagnac , N. Grau , S. V. Greene , M. Grosse Perdekamp , T. Gunji , H. Guragain , Y. Gu , T. Hachiya , J. S. Haggerty , K. I. Hahn , H. Hamagaki , J. Hanks , M. Harvey , S. Hasegawa , K. Hashimoto , R. Hayano , T. K. Hemmick , T. Hester , X. He , J. C. Hill , A. Hodges , R. S. Hollis , K. Homma , B. Hong , T. Hoshino , J. Huang , T. Ichihara , Y. Ikeda , K. Imai , Y. Imazu , M. Inaba , A. Iordanova , D. Isenhower , A. Isinhue , D. Ivanishchev , B. V. Jacak , S. J. Jeon , M. Jezghani , X. Jiang , Z. Ji , 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 , D. Kawall , A. V. Kazantsev , J. A. Key , V. Khachatryan , P. K. Khandai , A. Khanzadeev , A. Khatiwada , K. M. Kijima , C. Kim , D. J. Kim , E. -J. Kim , T. Kim , Y. -J. Kim , Y. K. Kim , D. Kincses , A. Kingan , E. Kistenev , J. Klatsky , D. Kleinjan , P. Kline , T. Koblesky , M. Kofarago , B. Komkov , J. Koster , D. Kotchetkov , D. Kotov , L. Kovacs , F. Krizek , B. Kurgyis , K. Kurita , M. Kurosawa , Y. Kwon , Y. S. Lai , J. G. Lajoie , D. Larionova , A. Lebedev , D. M. Lee , G. H. Lee , J. Lee , K. B. Lee , K. S. Lee , S. H. Lee , M. J. Leitch , M. Leitgab , B. Lewis , N. A. Lewis , S. H. Lim , M. X. Liu , X. Li , X. Li , D. A. Loomis , D. Lynch , S. Lökös , C. F. Maguire , T. Majoros , Y. I. Makdisi , M. Makek , A. Manion , V. I. Manko , E. Mannel , M. McCumber , P. L. McGaughey , D. McGlinchey , C. McKinney , A. Meles , M. Mendoza , B. Meredith , Y. Miake , T. Mibe , A. C. Mignerey , A. Milov , D. K. Mishra , J. T. Mitchell , M. Mitrankova , Iu. Mitrankov , S. Miyasaka , S. Mizuno , A. K. Mohanty , S. Mohapatra , M. M. Mondal , T. Moon , D. P. Morrison , M. Moskowitz , T. V. Moukhanova , B. Mulilo , 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 , S. Nelson , P. K. Netrakanti , M. Nihashi , T. Niida , R. Nouicer , N. Novitzky , T. Novák , G. Nukazuka , A. S. Nyanin , E. O'Brien , C. A. Ogilvie , J. Oh , H. Oide , K. Okada , M. Orosz , J. D. Osborn , A. Oskarsson , K. Ozawa , R. Pak , V. Pantuev , V. Papavassiliou , I. H. Park , J. S. Park , S. Park , S. K. Park , L. Patel , M. Patel , S. F. Pate , J. -C. Peng , W. Peng , D. V. Perepelitsa , G. D. N. Perera , D. Yu. Peressounko , C. E. PerezLara , J. Perry , R. Petti , C. Pinkenburg , R. P. Pisani , M. Potekhin , A. Pun , M. L. Purschke , H. Qu , P. V. Radzevich , J. Rak , N. Ramasubramanian , I. Ravinovich , K. F. Read , D. Reynolds , V. Riabov , Y. Riabov , E. Richardson , D. Richford , N. Riveli , D. Roach , S. D. Rolnick , M. Rosati , J. Runchey , M. S. Ryu , B. Sahlmueller , N. Saito , T. Sakaguchi , H. Sako , V. Samsonov , M. Sarsour , S. Sato , S. Sawada , K. Sedgwick , J. Seele , R. Seidl , Y. Sekiguchi , A. Sen , R. Seto , P. Sett , D. Sharma , A. Shaver , I. Shein , Z. Shi , M. Shibata , T. -A. Shibata , K. Shigaki , M. Shimomura , K. Shoji , P. Shukla , A. Sickles , C. L. Silva , D. Silvermyr , B. K. Singh , C. P. Singh , V. Singh , M. Skolnik , M. Slunečka , K. L. Smith , S. Solano , R. A. Soltz , W. E. Sondheim , S. P. Sorensen , I. V. Sourikova , P. W. Stankus , P. Steinberg , E. Stenlund , M. Stepanov , A. Ster , S. P. Stoll , M. R. Stone , T. Sugitate , A. Sukhanov , J. Sun , Z. Sun , R. Takahama , A. Takahara , A. Taketani , Y. Tanaka , K. Tanida , M. J. Tannenbaum , S. Tarafdar , A. Taranenko , E. Tennant , A. Timilsina , T. Todoroki , M. Tomášek , H. Torii , R. S. Towell , I. Tserruya , Y. Ueda , B. Ujvari , H. W. van Hecke , M. Vargyas , E. Vazquez-Zambrano , A. Veicht , J. Velkovska , M. Virius , V. Vrba , E. Vznuzdaev , R. Vértesi , X. R. Wang , Z. Wang , D. Watanabe , K. Watanabe , Y. Watanabe , Y. S. Watanabe , F. Wei , S. Whitaker , S. Wolin , C. P. Wong , C. L. Woody , M. Wysocki , B. Xia , Y. L. Yamaguchi , A. Yanovich , S. Yokkaichi , I. Yoon , I. Younus , Z. You , I. E. Yushmanov , W. A. Zajc , A. Zelenski , S. Zhou , L. Zou

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

Heavy flavor production is an ideal tool to study the properties of the Quark Gluon Plasma (QGP). The heavy flavor production at the Relativistic Heavy Ion Collider (RHIC) has its unique kinematic coverage and different production…

High Energy Physics - Experiment · Physics 2018-09-28 Xuan Li

Throughout the history of the RHIC physics program, questions concerning the dynamics of heavy quarks have generated much experimental and theoretical investigation. A major focus of the PHENIX experiment is the measurement of these quarks…

Nuclear Experiment · Physics 2015-05-30 J. Matthew Durham

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

Production and in-medium modification of hidden strange $\phi$ mesons are studied in proton-nucleus reactions - p+C, p+Cu and p+Pb - at 12 GeV/c, partially measured by the KEK E325 collaboration via the dilepton decay mode. This work is…

High Energy Physics - Phenomenology · Physics 2024-08-29 Philipp Gubler , Masaya Ichikawa , Taesoo Song , Elena Bratkovskaya

Polarized $p+p$ collisions provide insight into the structure of the nucleon. $A_N$ of eta mesons at forward rapidities are of particular interest, as asymmetries of other mesons observed both by PHENIX and other experiments show…

Nuclear Experiment · Physics 2019-08-13 David Kleinjan

We present measurements by the PHENIX experiment at RHIC of di-hadron pair production in \dAu collisions where the particles in the pair are varied across a wide range of pseudorapidity, out to $\eta = 3.8$. With di-hadrons, varying the…

Nuclear Experiment · Physics 2015-05-30 Mickey Chiu

We expose the current experimental and theoretical situation of the interesting case of the production of phi mesons in up to very high energy collisions of hadrons on both nucleon and nuclear targets, and we present a quantitavely good…

High Energy Physics - Phenomenology · Physics 2018-11-26 G. H. Arakelyan , C. Merino , Yu. M. Shabelski

The PHENIX experiment at RHIC measured $\omega$, $\eta$ and $K_{S}^{0}$-meson production at high $p_{T}$ in $p+p$, $d+Au$ and $Au+Au$ collisions at $\sqrt{s_{NN}}=200$ $GeV$. Measurements performed in different hadronic decay channels give…

Nuclear Experiment · Physics 2007-05-23 V. Riabov

Heavy quarks are good probes of the hot and dense medium created in relativistic heavy ion collisions since they are mainly generated early in the collision and interact with the medium in all collision stages. In addition, heavy flavor…

Nuclear Experiment · Physics 2019-08-13 Rachid Nouicer

Extensive experimental data from high-energy nucleus-nucleus collisions were recorded using the PHENIX detector at the Relativistic Heavy Ion Collider (RHIC). The comprehensive set of measurements from the first three years of RHIC…

Nuclear Experiment · Physics 2009-09-29 PHENIX Collaboration , K. Adcox