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Related papers: Direct Photon Measurements at PHENIX

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The PHENIX experiment has measured direct photons at $\sqrt{s_{NN}}$ = 200 GeV in $p+p$, $d$+Au and Au+Au collisions. For $p_{T}$ $<$ 4 GeV/$c$, the internal conversion into $e^{+}e^{-}$ pairs has been used to measure the direct photons in…

Nuclear Experiment · Physics 2019-08-14 B. Sahlmueller

Direct photons were measured with the PHENIX experiment in p+p, d+Au, and Au+Au at sqrt(s_NN) = 200 GeV. To tackle the p_T region below 5 GeV/c, direct photons were measured through their internal conversion into e^+e^- in Au+Au collisions.

Nuclear Experiment · Physics 2019-08-14 Stefan Bathe

Direct photons have been measured with the PHENIX experiment in Au+Au collisions at $\sqrt{s_\mathrm{NN}}$ = 200 GeV. The direct photon result obtained with PHENIX-EMCal up to 18 GeV/$c$ is consistent with the NLO pQCD calculation scaled by…

Nuclear Experiment · Physics 2008-11-26 Tadaaki Isobe

Direct photon spectra measured at small $p_T$ in p+p, d+Au and Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV are presented. Several measurement techniques including statistical subtraction, tagging, and internal and external conversion were…

Nuclear Experiment · Physics 2008-11-26 D. Peressounko

The PHENIX experiment has measured direct photons in $\sqrt{s_{NN}} = 200$ GeV Au+Au collisions and p+p collisions. The fraction of photons due to direct production in Au+Au collisions is shown as a function of $p_T$ and centrality. This…

Nuclear Experiment · Physics 2019-08-14 S. Mioduszewski

Results from the PHENIX experiment at RHIC on direct photon production in p+p, d+Au, and Au+Au collisions at sqrt(s_NN) = 200 GeV are presented. In p+p collisions, direct photon production at high p_T behaves as expected from perturbative…

Nuclear Experiment · Physics 2019-08-14 Stefan Bathe

Direct photon yield measured in p+p and d+Au collisions at \sqrt{s} = 200 GeV with the PHENIX experiment is presented and compared to pQCD predictions. In the case of p+p collisions both the inclusive and isolated direct photon production…

High Energy Physics - Experiment · Physics 2019-08-14 D. Peressounko

We present the first positive direct photon results in Au+Au at sqrt{s_NN} = 200 GeV along with initial p+p results at the same energy. The p+p result is found to be consistent with NLO perturbative QCD predictions within its large…

Nuclear Experiment · Physics 2009-11-10 Justin Frantz

The measurement of direct photons in s(NN)**1/2 = 200 GeV p+p and Au+Au collisions is presented. The signal is compared to NLO pQCD calculations, which, in case of Au+Au, are scaled with the number of underlying nucleon-nucleon collisions.…

Nuclear Experiment · Physics 2019-08-14 Stefan Bathe

Direct-photon measurements in p+p and Au+Au collisions at sqrt{s_{NN}} = 200 GeV from the PHENIX experiment are presented. The p+p results are found to be in good agreement with next-to-leading-order (NLO) perturbative QCD calculations.…

High Energy Physics - Experiment · Physics 2019-08-14 Klaus Reygers

The status of the search for direct photons in Au+Au collisions at sqrt{s_NN} = 130 GeV and sqrt{s_NN} = 200 GeV with the PHENIX experiment is presented. Within errors, no excess of direct photons was found in a first analysis pass done on…

Nuclear Experiment · Physics 2019-08-14 Klaus Reygers

We report the measurement of direct photons at midrapidity in Au+Au collisions at sqrt{s_NN} = 200 GeV. The direct photon signal was extracted for the transverse-momentum range of 4 GeV/c < p_T < 22 GeV/c, using a statistical method to…

Nuclear Experiment · Physics 2015-06-05 S. Afanasiev , C. Aidala , N. N. Ajitanand , Y. Akiba , A. Al-Jamel , J. Alexander , K. Aoki , L. Aphecetche , R. Armendariz , S. H. Aronson , R. Averbeck , T. C. Awes , B. Azmoun , V. Babintsev , 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 , 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 , S. Chernichenko , C. Y. Chi , J. Chiba , M. Chiu , I. J. Choi , T. Chujo , V. Cianciolo , C. R. Cleven , Y. Cobigo , B. A. Cole , M. P. Comets , M. Connors , P. Constantin , M. Csanád , T. Csörgő , T. Dahms , K. Das , G. David , H. Delagrange , A. Denisov , D. d'Enterria , A. Deshpande , E. J. Desmond , O. Dietzsch , A. Dion , J. L. Drachenberg , O. Drapier , A. Drees , A. K. Dubey , A. Durum , V. Dzhordzhadze , Y. V. Efremenko , J. Egdemir , A. Enokizono , H. En'yo , B. Espagnon , S. Esumi , D. E. Fields , F. Fleuret , S. L. Fokin , B. Forestier , Z. Fraenkel , J. E. Frantz , A. Franz , A. D. Frawley , Y. Fukao , S. -Y. Fung , S. Gadrat , F. Gastineau , M. Germain , A. Glenn , M. Gonin , J. Gosset , Y. Goto , R. Granier de Cassagnac , N. Grau , S. V. Greene , M. Grosse Perdekamp , T. Gunji , H. -Å. Gustafsson , T. Hachiya , A. Hadj Henni , J. S. Haggerty , M. N. Hagiwara , H. Hamagaki , H. Harada , E. P. Hartouni , K. Haruna , M. Harvey , E. Haslum , K. Hasuko , R. Hayano , X. He , M. Heffner , T. K. Hemmick , J. M. Heuser , H. Hiejima , J. C. Hill , R. Hobbs , M. Holmes , W. Holzmann , K. Homma , B. Hong , T. Horaguchi , M. G. Hur , T. Ichihara , H. Iinuma , K. Imai , J. Imrek , M. Inaba , 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 , M. Kaneta , J. H. Kang , T. Kawagishi , A. V. Kazantsev , S. Kelly , A. Khanzadeev , D. J. Kim , E. Kim , Y. -S. Kim , E. Kinney , Á. Kiss , E. Kistenev , A. Kiyomichi , C. Klein-Boesing , L. Kochenda , V. Kochetkov , B. Komkov , M. Konno , D. Kotchetkov , A. Kozlov , P. J. Kroon , G. J. Kunde , N. Kurihara , K. Kurita , M. J. Kweon , Y. Kwon , G. S. Kyle , R. Lacey , J. G. Lajoie , A. Lebedev , Y. Le Bornec , S. Leckey , D. M. Lee , M. K. Lee , M. J. Leitch , M. A. L. Leite , X. H. Li , H. Lim , A. Litvinenko , M. X. Liu , C. F. Maguire , Y. I. Makdisi , A. Malakhov , M. D. Malik , V. I. Manko , H. Masui , F. Matathias , M. C. McCain , P. L. McGaughey , Y. Miake , T. E. Miller , A. Milov , S. Mioduszewski , G. C. Mishra , J. T. Mitchell , D. P. Morrison , J. M. Moss , T. V. Moukhanova , D. Mukhopadhyay , J. Murata , S. Nagamiya , Y. Nagata , J. L. Nagle , M. Naglis , T. Nakamura , J. Newby , M. Nguyen , B. E. Norman , A. S. Nyanin , J. Nystrand , E. O'Brien , C. A. Ogilvie , H. Ohnishi , I. D. Ojha , K. Okada , O. O. Omiwade , A. Oskarsson , I. Otterlund , K. Ozawa , 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. Qu , J. Rak , I. Ravinovich , K. F. Read , 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 , V. Samsonov , H. D. Sato , S. Sato , S. Sawada , V. Semenov , R. Seto , D. Sharma , T. K. Shea , I. Shein , T. -A. Shibata , K. Shigaki , M. Shimomura , T. Shohjoh , K. Shoji , A. Sickles , C. L. Silva , D. Silvermyr , K. S. Sim , C. P. Singh , V. Singh , S. Skutnik , 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 , J. Tojo , 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. van Hecke , J. Velkovska , R. Vértesi , A. A. Vinogradov , E. Vznuzdaev , M. Wagner , X. R. Wang , Y. Watanabe , J. Wessels , S. N. White , N. Willis , D. Winter , C. L. Woody , M. Wysocki , W. Xie , A. Yanovich , S. Yokkaichi , G. R. Young , I. Younus , I. E. Yushmanov , W. A. Zajc , O. Zaudtke , C. Zhang , J. Zimányi , L. Zolin

Results on direct photon measurements from the PHENIX experiment at RHIC are presented. The direct photon yields for $p_T>$6 GeV/$c$ as a function of centrality in Au-Au collisions at $\sqrt{s_{NN}}$=200 GeV are found to be consistent with…

Nuclear Experiment · Physics 2019-08-14 T. Sakaguchi

When studying the initial state and evolution of the matter created in relativistic heavy ion collisions, high-pT direct photons are a powerful probe. They are created in initial hard processes and in parton fragmentation, and possibly in…

Nuclear Experiment · Physics 2008-11-26 Tadaaki Isobe

The PHENIX collaboration has measured low momentum direct photon radiation in Au+Au collisions at 200 GeV, 62.4 GeV and 39 GeV, in Cu+Cu at 200 GeV as well as in p+p, p+Au and d+Au at $\sqrt{s_{NN}} =$ 200 GeV. In these measurements PHENIX…

Nuclear Experiment · Physics 2018-12-27 Vladimir Khachatryan

The measurements of direct photons in $1.0 < p_{T} < 5.0 $GeV/$c$ for p+p and Au+Au collisions have been made through the virtual photon method at PHENIX. The fraction of the virtual direct photon component to the inclusive $e^{+}e^{-}$…

Nuclear Experiment · Physics 2019-08-13 Yorito Yamaguchi

As a colorless probe, direct photons balance the $p_T$ of the away-side jet at leading order. Direct photon-hadron correlations are thus an excellent probe for nuclear structure and QCD effects, including parton energy loss in the…

High Energy Physics - Experiment · Physics 2019-08-13 J. D. Osborn

Direct photon production in Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV has been measured in the $p_T$ range of 1$<$$p_T$$<$5 GeV/$c$. The yield as acfunction of centrality is in agreement with published data of the RHIC 2002 run, and with…

Nuclear Experiment · Physics 2009-11-11 Takao Sakaguchi

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

The versatility of RHIC allowed the PHENIX collaboration to measure low momentum direct photons from small systems, such as p+p, p+A, d+Au at $\sqrt{s_{NN}} = $200 GeV as well as from large A+A systems, such as Au+Au and Cu+Cu at 200 GeV…

Nuclear Experiment · Physics 2019-02-20 Vladimir Khachatryan
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