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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

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

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

Heavy quarks (charm and bottom) are good probes of the hot and dense medium created in relativistic heavy ion collisions since they are mainly generated at the beginning of collisions and interact with the media in all collision stages. In…

Nuclear Experiment · Physics 2019-08-13 M. L. Brooks

The PHENIX experiment at RHIC has measured single electron spectra in proton-proton, deuteron-gold and gold-gold collisions at sqrt(s_NN)=200 GeV. The photonic contribution (photon conversions and Daltiz decays) is subtracted from the…

Nuclear Experiment · Physics 2009-11-10 Sean Kelly

The measurement of single leptons from the semi-leptonic decay of heavy-flavor hadrons has long been a means for studying heavy-quark production. PHENIX has measured single muons in pp collisions at forward rapidity and single electrons in…

Nuclear Experiment · Physics 2019-08-13 Donald Hornback

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

Heavy quarks are an ideal probe of the quark gluon plasma created in heavy ion collisions. They are produced in the initial hard scattering and therefore experience the full evolution of the medium. PHENIX has previously measured the…

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

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

Transverse momentum (p^e_T) spectra of electrons from semileptonic weak decays of heavy flavor mesons in the range of 0.3 < p^e_T < 9.0 GeV/c have been measured at mid-rapidity (|eta| < 0.35) by the PHENIX experiment at the Relativistic…

Nuclear Experiment · Physics 2016-08-14 A. Adare , S. Afanasiev , C. Aidala , N. N. Ajitanand , Y. Akiba , H. Al-Bataineh , J. Alexander , A. Al-Jamel , K. Aoki , L. Aphecetche , R. Armendariz , S. H. Aronson , J. Asai , E. T. Atomssa , R. Averbeck , T. C. Awes , B. Azmoun , V. Babintsev , G. Baksay , L. Baksay , A. Baldisseri , K. N. Barish , P. D. Barnes , B. Bassalleck , S. Bathe , S. Batsouli , V. Baublis , F. Bauer , A. Bazilevsky , S. Belikov , R. Bennett , Y. Berdnikov , A. A. Bickley , M. T. Bjorndal , J. G. Boissevain , H. Borel , K. Boyle , M. L. Brooks , D. S. Brown , D. Bucher , H. Buesching , V. Bumazhnov , G. Bunce , J. M. Burward-Hoy , S. Butsyk , S. Campbell , J. -S. Chai , B. S. Chang , J. -L. Charvet , S. Chernichenko , J. Chiba , C. Y. Chi , M. Chiu , I. J. Choi , T. Chujo , P. Chung , A. Churyn , V. Cianciolo , C. R. Cleven , Y. Cobigo , B. A. Cole , M. P. Comets , P. Constantin , M. Csanád , T. Csörgő , T. Dahms , K. Das , G. David , M. B. Deaton , K. Dehmelt , H. Delagrange , A. Denisov , D. d'Enterria , A. Deshpande , E. J. Desmond , O. Dietzsch , A. Dion , M. Donadelli , J. L. Drachenberg , O. Drapier , A. Drees , A. K. Dubey , A. Durum , V. Dzhordzhadze , Y. V. Efremenko , J. Egdemir , F. Ellinghaus , W. S. Emam , A. Enokizono , H. En'yo , B. Espagnon , S. Esumi , K. O. Eyser , D. E. Fields , M. FingerJr. , 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. GranierdeCassagnac , N. Grau , S. V. Greene , M. Grosse Perdekamp , T. Gunji , H. -Å. Gustafsson , T. Hachiya , A. Henni , Hadj , C. Haegemann , J. S. Haggerty , M. N. Hagiwara , H. Hamagaki , 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 , M. G. Hur , T. Ichihara , K. Imai , M. Inaba , Y. Inoue , D. Isenhower , L. Isenhower , M. Ishihara , T. Isobe , M. Issah , A. Isupov , B. V. Jacak , J. Jia , J. Jin , O. Jinnouchi , B. M. Johnson , K. S. Joo , D. Jouan , F. Kajihara , S. Kametani , N. Kamihara , J. Kamin , M. Kaneta , J. H. Kang , H. Kanou , T. Kawagishi , D. Kawall , A. V. Kazantsev , S. Kelly , A. Khanzadeev , J. Kikuchi , D. H. Kim , D. J. Kim , E. 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 , D. Kotchetkov , A. Kozlov , A. Král , A. Kravitz , P. J. Kroon , J. Kubart , G. J. Kunde , N. Kurihara , K. Kurita , M. J. Kweon , Y. Kwon , G. S. Kyle , R. Lacey , Y. -S. Lai , J. G. Lajoie , A. Lebedev , Y. LeBornec , S. Leckey , D. M. Lee , M. K. Lee , T. Lee , M. J. Leitch , M. A. L. Leite , B. Lenzi , H. Lim , T. Liška , A. Litvinenko , 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 , Y. Mao , L. Mašek , H. Masui , F. Matathias , M. C. McCain , M. McCumber , P. L. McGaughey , Y. Miake , P. Mikeš , K. Miki , T. E. Miller , A. Milov , S. Mioduszewski , G. C. Mishra , M. Mishra , J. T. Mitchell , M. Mitrovski , A. Morreale , D. P. Morrison , J. M. Moss , T. V. Moukhanova , D. Mukhopadhyay , J. Murata , S. Nagamiya , Y. Nagata , J. L. Nagle , M. Naglis , I. Nakagawa , Y. Nakamiya , T. Nakamura , K. Nakano , J. Newby , M. Nguyen , B. E. Norman , R. Nouicer , A. S. Nyanin , J. Nystrand , E. O'Brien , S. X. Oda , C. A. Ogilvie , H. Ohnishi , I. D. Ojha , H. Okada , K. Okada , M. Oka , O. O. Omiwade , A. Oskarsson , I. Otterlund , M. Ouchida , K. Ozawa , R. Pak , D. Pal , A. P. T. Palounek , V. Pantuev , V. Papavassiliou , J. Park , W. J. Park , S. F. Pate , H. Pei , J. -C. Peng , H. Pereira , V. Peresedov , D. Yu. Peressounko , C. Pinkenburg , R. P. Pisani , M. L. Purschke , A. K. Purwar , H. Rak , J. Qu , A. Rakotozafindrabe , I. Ravinovich , K. F. Read , S. Rembeczki , M. Reuter , K. Reygers , V. Riabov , Y. Riabov , G. Roche , A. Romana , M. Rosati , S. S. E. Rosendahl , P. Rosnet , P. Rukoyatkin , V. L. Rykov , S. S. Ryu , B. Sahlmueller , N. Saito , T. Sakaguchi , S. Sakai , H. Sakata , V. Samsonov , H. D. Sato , S. Sato , S. Sawada , 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 , A. Sickles , C. L. Silva , D. Silvermyr , C. Silvestre , K. S. Sim , C. P. Singh , V. Singh , S. Skutnik , M. Slunečka , 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 , J. P. Sullivan , J. Sziklai , T. Tabaru , S. Takagi , E. M. Takagui , A. Taketani , K. H. Tanaka , Y. Tanaka , K. Tanida , M. J. Tannenbaum , A. Taranenko , P. Tarján , T. L. Thomas , M. Togawa , A. Toia , J. Tojo , L. Tomášek , H. Torii , R. S. Towell , V-N. Tram , I. Tserruya , Y. Tsuchimoto , S. K. Tuli , H. Tydesjö , N. Tyurin , C. Vale , H. Valle , H. W. vanHecke , J. Velkovska , R. Vertesi , A. A. Vinogradov , M. Virius , V. Vrba , E. Vznuzdaev , M. Wagner , D. Walker , X. R. Wang , Y. Watanabe , J. Wessels , S. N. White , N. Willis , D. Winter , C. L. Woody , M. Wysocki , W. Xie , Y. L. Yamaguchi , A. Yanovich , Z. Yasin , J. Ying , S. Yokkaichi , G. R. Young , I. Younus , I. E. Yushmanov , W. A. Zajc , O. Zaudtke , C. Zhang , S. Zhou , J. Zimányi , L. Zolin

The PHENIX experiment has measured mid-rapidity transverse momentum spectra (0.4 < p_T < 5.0 GeV/c) of electrons as a function of centrality in Au+Au collisions at sqrt(s_NN)=200 GeV. Contributions from photon conversions and from light…

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

Charm and bottom quarks are formed predominantly by gluon fusion in the initial hard scatterings at RHIC, making them good probes of the full medium evolution. Previous measurements at RHIC have shown large suppression and azimuthal…

Nuclear Experiment · Physics 2015-06-22 Sanghoon Lim

The PHENIX experiment has measured single electron spectra at RHIC in proton-proton (p-p), deuteron-gold (d-Au), and gold-gold (Au-Au) collisions at an available energy per nucleon-nucleon pair of sqrt{s_NN} = 200 GeV. Contributions from…

Nuclear Experiment · Physics 2019-08-14 Ralf Averbeck

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

Heavy quarks are a valuable probe of the hot, dense medium created in a heavy ion collision, and are an important test of proposed mechanisms of energy loss. It was discovered that single non-photonic electrons are suppressed at a similar…

Nuclear Experiment · Physics 2019-08-13 Tatia Engelmore

In recent years, PHENIX has studied many important observables related to heavy-flavor physics through their leptonic decay measurements including the invariant yield of electrons from nonphotonic sources, and prompt single muons, both of…

Nuclear Experiment · Physics 2019-08-21 Marisilvia Donadelli

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

Hadrons carrying heavy quarks, i.e. charm or bottom, are important probes of the hot and dense medium created in relativistic heavy ion collisions. Heavy quark-antiquark pairs are mainly produced in initial hard scattering processes of…

Nuclear Experiment · Physics 2015-12-30 Rachid Nouicer

PHENIX has measured direct photons in p+p and Au+Au collisions at sqrt{s_{NN}}=200 GeV. The p+p measurement is in good agreement with pQCD expectations. The nuclear modification factor in Au+Au is found to be consistent with unity for all…

Nuclear Experiment · Physics 2019-08-13 Baldo Sahlmueller

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
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