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

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One of the main objectives of the NA61/SHINE experiment at the CERN SPS is to study properties of strongly interacting matter. This paper presents new results on observables relevant for this part of the NA61/SHINE programme. These include…

High Energy Physics - Experiment · Physics 2019-08-21 Antoni Marcinek

The measurement of the nuclear modification factor ($R_{\rm AA}$) for heavy-flavor production in heavy-ion collisions tests predictions for cold- and hot-nuclear-matter effects. Heavy-flavor production in \pp\ collisions tests pQCD…

Nuclear Experiment · Physics 2019-08-13 K. F. Read

Hadronic resonances serve as unique probes in the study of the hot and dense nuclear matter produced in heavy-ion collisions. Properties of the hadronic phase of the collision can be extracted from measurements of the suppression of…

Nuclear Experiment · Physics 2019-08-13 A. G. Knospe

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

Measurement of neutral pions and direct photons are closely connected experimentally, on the other hand they probe quite different aspects of relativistic heavy ion collisions. In this short review of the $\pi^0$ results from the PHENIX…

Nuclear Experiment · Physics 2010-02-09 G. David

The observation of meson and baryon grouping in the $R_{CP}$ and $v_2$ measurements at intermediate $p_T$ has been interpreted as a manifestation of bulk partonic matter hadronization through multi-parton dynamics such as recombination of…

Nuclear Experiment · Physics 2008-11-26 Xiangzhou Cai

We review recent results on hard observables in p+p, d+A and A+A collisions obtained by the PHENIX experiment. Emphasis is put on those measurements that provide insight into the properties of hot QCD media expected to be created in…

Nuclear Experiment · Physics 2019-08-14 D. Peressounko

The measurement of light vector meson production (\rho, \omega, \phi) in pp collisions provides insight into soft Quantum Chromodynamics (QCD) processes in the LHC energy range. Calculations in this regime are based on QCD inspired…

High Energy Physics - Experiment · Physics 2012-09-25 Elisa Incani

The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of phi meson production in the K+K- decay channel at midrapidity in p+p, d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV.…

Nuclear Experiment · Physics 2011-02-23 PHENIX Collaboration , A. Adare , S. Afanasiev , C. Aidala , N. N. Ajitanand , Y. Akiba , H. Al-Bataineh , J. Alexander , A. Al-Jamel , A. Angerami , K. Aoki , L. Aphecetche , Y. Aramaki , R. Armendariz , S. H. Aronson , J. Asai , E. T. Atomssa , R. Averbeck , T. C. Awes , B. Azmoun , V. Babintsev , M. Bai , G. Baksay , L. Baksay , A. Baldisseri , K. N. Barish , P. D. Barnes , B. Bassalleck , A. T. Basye , S. Bathe , S. Batsouli , V. Baublis , F. Bauer , C. Baumann , A. Bazilevsky , S. Belikov , R. Belmont , R. Bennett , A. Berdnikov , Y. Berdnikov , J. H. Bhom , A. A. Bickley , M. T. Bjorndal , D. S. Blau , J. G. Boissevain , J. S. Bok , H. Borel , N. Borggren , K. Boyle , M. L. Brooks , D. S. Brown , D. Bucher , H. Buesching , V. Bumazhnov , G. Bunce , J. M. Burward-Hoy , S. Butsyk , S. Campbell , A. Caringi , N. Cassano , J. -S. Chai , B. S. Chang , J. -L. Charvet , C. -H. Chen , S. Chernichenko , J. Chiba , C. Y. Chi , M. Chiu , I. J. Choi , J. B. Choi , R. K. Choudhury , P. Christiansen , T. Chujo , P. Chung , A. Churyn , O. Chvala , V. Cianciolo , Z. Citron , C. R. Cleven , Y. Cobigo , B. A. Cole , M. P. Comets , Z. Conesa del Valle , M. Connors , P. Constantin , M. Csanad , T. Csorgo , T. Dahms , S. Dairaku , I. Danchev , K. Das , A. Datta , G. David , M. K. Dayananda , M. B. Deaton , K. Dehmelt , H. Delagrange , A. Denisov , D. d'Enterria , A. Deshpande , E. J. Desmond , K. V. Dharmawardane , O. Dietzsch , A. Dion , M. Donadelli , L. D Orazio , J. L. Drachenberg , O. Drapier , A. Drees , K. A. Drees , A. K. Dubey , J. M. Durham , A. Durum , D. Dutta , V. Dzhordzhadze , S. Edwards , Y. V. Efremenko , J. Egdemir , F. Ellinghaus , W. S. Emam , T. Engelmore , A. Enokizono , H. En'yo , B. Espagnon , S. Esumi , K. O. Eyser , B. Fadem , D. E. Fields , M. Finger , M. Finger , F. Fleuret , S. L. Fokin , B. Forestier , Z. Fraenkel , J. E. Frantz , A. Franz , A. D. Frawley , K. Fujiwara , Y. Fukao , S. -Y. Fung , T. Fusayasu , S. Gadrat , I. Garishvili , F. Gastineau , M. Germain , A. Glenn , H. Gong , M. Gonin , J. Gosset , Y. Goto , R. Granier de Cassagnac , N. Grau , S. V. Greene , G. Grim , M. Grosse Perdekamp , T. Gunji , H. -A. Gustafsson , T. Hachiya , A. Hadj Henni , C. Haegemann , J. S. Haggerty , M. N. Hagiwara , K. I. Hahn , H. Hamagaki , J. Hamblen , J. Hanks , R. Han , H. Harada , E. P. Hartouni , K. Haruna , M. Harvey , E. Haslum , K. Hasuko , R. Hayano , M. Heffner , T. K. Hemmick , T. Hester , J. M. Heuser , X. He , H. Hiejima , J. C. Hill , R. Hobbs , M. Hohlmann , M. Holmes , W. Holzmann , K. Homma , B. Hong , T. Horaguchi , D. Hornback , S. Huang , M. G. Hur , T. Ichihara , R. Ichimiya , H. Iinuma , Y. Ikeda , K. Imai , M. Inaba , Y. Inoue , D. Isenhower , L. Isenhower , M. Ishihara , T. Isobe , M. Issah , A. Isupov , D. Ivanischev , Y. Iwanaga , B. V. Jacak , J. Jia , X. Jiang , J. Jin , O. Jinnouchi , B. M. Johnson , T. Jones , K. S. Joo , D. Jouan , D. S. Jumper , F. Kajihara , S. Kametani , N. Kamihara , J. Kamin , M. Kaneta , J. H. Kang , H. Kanou , J. Kapustinsky , K. Karatsu , M. Kasai , T. Kawagishi , D. Kawall , M. Kawashima , A. V. Kazantsev , S. Kelly , T. Kempel , A. Khanzadeev , K. M. Kijima , J. Kikuchi , A. Kim , B. I. Kim , D. H. Kim , D. J. Kim , E. J. Kim , E. Kim , Y. -J. Kim , Y. -S. Kim , E. Kinney , A. Kiss , E. Kistenev , A. Kiyomichi , J. Klay , C. Klein-Boesing , L. Kochenda , V. Kochetkov , B. Komkov , M. Konno , J. Koster , D. Kotchetkov , D. Kotov , A. Kozlov , A. Kral , A. Kravitz , P. J. Kroon , J. Kubart , G. J. Kunde , N. Kurihara , K. Kurita , M. Kurosawa , M. J. Kweon , Y. Kwon , G. S. Kyle , R. Lacey , Y. S. Lai , J. G. Lajoie , A. Lebedev , Y. Le Bornec , S. Leckey , D. M. Lee , J. Lee , K. B. Lee , K. S. Lee , M. K. Lee , T. Lee , M. J. Leitch , M. A. L. Leite , B. Lenzi , P. Lichtenwalner , P. Liebing , H. Lim , L. A. Linden Levy , T. Liska , A. Litvinenko , H. Liu , M. X. Liu , X. Li , X. H. Li , B. Love , D. Lynch , C. F. Maguire , Y. I. Makdisi , A. Malakhov , M. D. Malik , V. I. Manko , E. Mannel , Y. Mao , L. Masek , H. Masui , F. Matathias , M. C. McCain , M. McCumber , P. L. McGaughey , N. Means , B. Meredith , Y. Miake , T. Mibe , A. C. Mignerey , P. Mikes , K. Miki , T. E. Miller , A. Milov , S. Mioduszewski , G. C. Mishra , M. Mishra , J. T. Mitchell , M. Mitrovski , A. K. Mohanty , H. J. Moon , Y. Morino , A. Morreale , D. P. Morrison , J. M. Moss , T. V. Moukhanova , D. Mukhopadhyay , T. Murakami , J. Murata , S. Nagamiya , Y. Nagata , J. L. Nagle , M. Naglis , M. I. Nagy , I. Nakagawa , Y. Nakamiya , K. R. Nakamura , T. Nakamura , K. Nakano , S. Nam , J. Newby , M. Nguyen , M. Nihashi , B. E. Norman , R. Nouicer , A. S. Nyanin , J. Nystrand , C. Oakley , E. O'Brien , S. X. Oda , C. A. Ogilvie , H. Ohnishi , I. D. Ojha , K. Okada , M. Oka , O. O. Omiwade , Y. Onuki , A. Oskarsson , I. Otterlund , M. Ouchida , K. Ozawa , R. Pak , D. Pal , A. P. T. Palounek , V. Pantuev , V. Papavassiliou , I. H. Park , J. Park , S. K. Park , W. J. Park , S. F. Pate , H. Pei , J. -C. Peng , H. Pereira , V. Peresedov , D. Yu. Peressounko , R. Petti , C. Pinkenburg , R. P. Pisani , M. Proissl , M. L. Purschke , A. K. Purwar , H. Qu , J. Rak , A. Rakotozafindrabe , I. Ravinovich , K. F. Read , S. Rembeczki , M. Reuter , K. Reygers , V. Riabov , Y. Riabov , E. Richardson , D. Roach , G. Roche , S. D. Rolnick , A. Romana , M. Rosati , C. A. Rosen , S. S. E. Rosendahl , P. Rosnet , P. Rukoyatkin , P. Ruzicka , V. L. Rykov , S. S. Ryu , B. Sahlmueller , N. Saito , T. Sakaguchi , S. Sakai , K. Sakashita , H. Sakata , V. Samsonov , S. Sano , H. D. Sato , S. Sato , T. Sato , S. Sawada , K. Sedgwick , J. Seele , R. Seidl , V. Semenov , R. Seto , D. Sharma , T. K. Shea , I. Shein , A. Shevel , T. -A. Shibata , K. Shigaki , M. Shimomura , T. Shohjoh , K. Shoji , P. Shukla , A. Sickles , C. L. Silva , D. Silvermyr , C. Silvestre , K. S. Sim , B. K. Singh , C. P. Singh , V. Singh , S. Skutnik , M. Slunecka , W. C. Smith , A. Soldatov , R. A. Soltz , W. E. Sondheim , S. P. Sorensen , I. V. Sourikova , F. Staley , P. W. Stankus , E. Stenlund , M. Stepanov , A. Ster , S. P. Stoll , T. Sugitate , C. Suire , A. Sukhanov , J. P. Sullivan , J. Sziklai , T. Tabaru , S. Takagi , E. M. Takagui , A. Taketani , R. Tanabe , K. H. Tanaka , Y. Tanaka , S. Taneja , K. Tanida , M. J. Tannenbaum , S. Tarafdar , A. Taranenko , P. Tarjan , H. Themann , D. Thomas , T. L. Thomas , M. Togawa , A. Toia , J. Tojo , L. Tomasek , H. Torii , R. S. Towell , V-N. Tram , I. Tserruya , Y. Tsuchimoto , S. K. Tuli , H. Tydesjo , N. Tyurin , C. Vale , H. Valle , H. W. van Hecke , E. Vazquez-Zambrano , A. Veicht , J. Velkovska , R. Vertesi , A. A. Vinogradov , M. Virius , V. Vrba , E. Vznuzdaev , M. Wagner , D. Walker , X. R. Wang , D. Watanabe , K. Watanabe , Y. Watanabe , F. Wei , J. Wessels , S. N. White , N. Willis , D. Winter , C. L. Woody , R. M. Wright , M. Wysocki , W. Xie , Y. L. Yamaguchi , K. Yamaura , R. Yang , A. Yanovich , Z. Yasin , J. Ying , S. Yokkaichi , G. R. Young , I. Younus , Z. You , I. E. Yushmanov , W. A. Zajc , O. Zaudtke , C. Zhang , S. Zhou , J. Zimanyi , L. Zolin

We present the first elliptic flow, $v_{2}$, measurement for the $\phi$-meson in Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV. At low $p_{T}$ (<2 GeV/c), the $v_{2}$ is consistent with mass ordering expected from hydrodynamics, while at…

Nuclear Experiment · Physics 2009-11-11 Sarah-Louise Blyth

The heavy ion physics approach to global event characterization has led us to instrument the forward region in the PHENIX experiment at RHIC. In heavy ion collisions this coverage yields a measurement of the "spectator" energy and its…

Nuclear Experiment · Physics 2008-11-26 Sebastian N. White

The PHENIX experiment at RHIC measured the omega-meson production in the range of pT from 2.5 GeV/c to 9.5 GeV/c in p+p and d+Au collision systems at sqrt{s_{NN}}=200 GeV. We present the consistent results of two independent measurements in…

High Energy Physics - Experiment · Physics 2007-05-23 V. Ryabov

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

We present the first results of meson production in the K^+K^- decay channel from Au+Au collisions at sqrt(s_NN) = 200 GeV as measured at mid-rapidity by the PHENIX detector at RHIC. Precision resonance centroid and width values are…

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

To interpret the measurements in heavy-ion collisions at the Relativistic Heavy-Ion Collider (RHIC) it is crucial to understand the initial state of the colliding gold (Au) nuclei. The parton distribution in Au nuclei is modified compared…

Nuclear Experiment · Physics 2019-08-13 Baldo Sahlmueller

The properties of the phi-meson have been measured via its e+e- and K+K- decay channels in Au+Au collisions at sqrt{s_NN} = 200 GeV by the PHENIX experiment. The preliminary yields and temperatures derived for the minimum bias and several…

Nuclear Experiment · Physics 2007-05-23 Alexander Kozlov

We report the first results of the nuclear modification factors and elliptic flow of the phi mesons measured by the PHENIX experiment at RHIC in high luminosity Au+Au collisions at sqrt(sNN) = 200 GeV. The nuclear modification factors R_AA…

High Energy Physics - Experiment · Physics 2016-08-31 Dipali Pal

This contribution presents the latest results on heavy quarkonia (j/psi and upsilon) production in d+A and A+A collisions at RHIC at a center of mass energy per nucleon-nucleon collision sqrt(s_NN) = 200 GeV, measured by the PHENIX…

Nuclear Experiment · Physics 2019-08-13 Hugo Pereira Da Costa

I report on results from the PHENIX collaboration for the first RHIC run, where gold ions were collided at $\sqrt{s_{NN}}=130 GeV$. In order to study initial conditions, PHENIX has measured the ratio between anti-protons and protons, the…

High Energy Physics - Phenomenology · Physics 2019-08-14 Kenneth N. Barish

The pi0 meson has been a crucial proble for observing jet quenching in ultrarelativistic heavy-ion collisions at RHIC. Measurements of the eta meson in the same collisions have also shed light on a possible dependence of the observed…

Nuclear Experiment · Physics 2019-08-21 B. Sahlmueller