Overview of PHENIX results from the first RHIC run

Zajc, W. A.; Adcox, K.; Adler, S. S.; Ajitanand, N. N.; Akiba, Y.; Alexander, J.; Allen, W.C.; Alley, G.T.; Aphecetche, L.; Arai, Y.; Archuleta, J.B.; Archuleta, J.; Armijo, V.; Aronson, S. H.; Atatekin, I.; Autrey, Daniel; Averbeck, R.; Awes, T. C.; Barishi, K. N.; Barnes, P. D.; Barretto, J.; Bassalleck, B.; Bathe, S.; Baublis, V.; Bazilevsky, A.; Behrendt, Jörg; Беликов, С.; Bellaiche, F.; Belyaev, S. T.; Bennett, M. J.; Berdnikov, Y.; Bluhm, D. D.; Bobrek, M.; Boissevain, J. G.; Boose, S.; Botelho, S.; Branning, J.M.; Britton, C.L.; Brooks, M. L.; Brown, D. S.; Bruner, N.; Bryan, W.L.; Bucher, D.; Buesching, H.; Bumazhnov, V.; Bunce, G.; Burward-Hoy, J. M.; Butsyk, S.; Cafferty, M.M.; Carey, T. A.; Chand, P.; Chang, James; Chang, W. C.; Chappell, R.B.; Chavez, L. L.; Chernichenko, S.; Y., C.; Chiba, J.; Chiu, M.; Choudhury, R. K.; Christ, T.; Chujo, T.; Chung, M.; Chung, P.; Cianciolo, V.; Cole, B.; Crook, D.W.; Cunitz, H.; d’Enterria, D.; Daniel, S. Q.; David, G.; Delagrange, H.; Denisov, A.; Deshpando, A.; Desmond, E. J.; Dietzsch, O.; Dinesh, B. V.; Drees, A.; Durum, A.; Dutta, D.; Ebisu, K.; Echave, M.A.; Efremenko, Y. V.; Chenawi, K. El; Emery, M.S.; En’yo, H.; Ericson, M.; Esumi, S.; Evseev, V.A.; Ewell, L.; Ferdousi, T.; Fields, D. E.; Fokin, S.; Fraenkel, Z.; Frank, S.S.; Frawley, A. D.; Fried, J.; Fung, S. Y.; Gannon, J.; Garpman, S.; Gee, Timothy F.; Ghosh, Tarun Kanti; Giannotti, R.; Gil, Y.; Glenn, A.; Godot, A. L.; Goto, Yuji; Greene, S.; Perdekamp, M. Grosse; Gupta, S. K.; Guryn, W.; Gustafsson, H.-Å.; Haggerty, J. S.; Hahn, S.; Hamagaki, H.; Hanson, A. G.; Hara, Hiroshi; Harder, J.; Hart, Greg; Hartouni, E. P.; Hayano, R. S.; Hayashi, Naoki; He, X. Q.; Heine, N.; Heistermann, F.; Hemmick, T. K.; Houser, J.; Hibino, M.; Hicks, J.S.; Hill, J. C.; Ho, D. S.; Homma, K.; Hong, B.; Hoover, A.; Hutchins, J.R.; Hutter, R.; Ichihara, T.; Imai, K.; Ippolitov, M.; Ishihara, M.; Jacak, B.; Jagadish, U.; Jang, W. Y.; Jia, J.; Johnson, B. M.; Johnson, S. C.; Jones, J.P.; Joo, K. S.; Kahn, S. J.; Kametani, S.; Kamyshkov, Yu.; Kandasamy, A.; Kang, J. H.; Kann, M.; Kapoor, S. S.; Karadjev, K.; Kato, S.; Kelley, M.; Kelly, S.; Kennedy, M.; Khachaturov, B.; Khanzadeev, A.; Khomoutnikov, A.; Kikuchi, Jun; Kim, D. J.; Kim, H. J.; Kim, S. Y.; Kim, Y. G.; Kinnison, W. W.; Kistenev, E.; Kiyomichi, A.; Klein-Boesing, Christian; Klinksick, S.; Kochcnda, L.; Kochetkov, D.; Kochetkov, V.; Koehler, D.; Kohama, T.; Komkov, B.; Kozlov, A.; Козлов, В. В.; Kravtsov, P.; Kroon, P. J.; Kuriatkov, V.V.; Kurita, K.; Kweon, M. J.; Kwon, Y.; Kyle, G. S.; Lacey, R.; Lajoie, J. G.; Lauret, J.; Лебедев, А.Н.; Lebedev, V.; Lee, D. M.; Leitch, M. J.; Li, X. H.; Li, Z.; Lim, D. J.; Lind, Randall F.; Lux, M. X.; Liu, X.; Liu, Z.; Maguire, C.; Mahon, J. R.; Makdisi, Y. I.; Manko, V.; Mao, Y.; Marek, Lukáš; Mark, S. K.; Markacs, S.; Markushin, D.G.; Martı́nez, G.; Marx, M.; Masaike, A.; Matathias, F.; Matsumoto, T.; McGahern, W.; McGaughey, P. L.; McMillan, D. E.; Melnikov, E.; Merschmeycr, M.; Messer, F.; Messer, M.; Miake, Y.; Miftakhov, N.; Miller, T. E.; Milov, A.; Mioduszewski, S.; Mischke, R. E.; Mlshra, G. C.; Mitchell, J. T.; Mohanty, A. K.; Montoya, B.C.; Moore, James A.; Morrison, D. P.; Moscone, C.G.; Moss, J. M.; Mühlbacher, F.; Muniruzzaman, M.; Murata, J.; Nagamiya, S.; Nagasaka, Y.; Nagle, J. L.; Nakada, Y.; Nandi, B. K.; Newby, J.; Nikkinen, L.; Nikolaev, S.; Nilsson, P.; Nishimura, S.; Nyanin, A.; Nystrand, J.; O’Brien, E.; Ogilvie, C. A.; Ohnìshì, H.; Ojha, I. D.; Ono, M.; Onuchìn, V.; Öskarsson, A.; Österman, L.; Otterlund, I.; Oyama, K.; Paffrath, L.; Palounek, A. P.T.; Pancake, C.; Pantuev, V.; Papavassiliou, V.; Pasmantirer, B.; Pate, S. F.; Pearson, C.; Peitzmann, T.; Petridis, Athanasios; Pinkenburg, C.; Pisani, R. P.; Pitukhin, P. V.; Plášil, F.; Pollack, M.; Pope, K.; Prigl, R.; Purschke, M. L.; Rankowitz, S.; Ravinovich, I.; Read, K. F.; Reygers, K.; Riabov, V.; Riabov, Y.; Richardson, G.; Robinson, S.; Rosati, M.; Roschin, E.; Rose, A.; Ruggiero, R.; Ryu, S. S.; Saito, N.; Sakaguchi, A.; Sakaguchi, T.; Sako, H.; Sakuma, T.; Samsonov, V.; Sangster, T. C.; Santo, R.; Sato, H.; Sato, Susumu; Sawada, S.; Schlei, B. R.; Schütz, Y.; Semenov, V.; Seto, R.; Shea, T. K.; Shein, I.; Shibata, T. A.; Shigaki, K.; Shiina, T.; Shin, Y. H.; Sibiriak, I.; Silvermyr, D.; Sim, K. S.; Gillo, J. S.; Singh, Captain R.; Singh, V.; Sippach, F.W.; Sivertz, M.; Skank, H.D.; Sleege, Gary; Smith, Douglas E.; Smith, Geoffrey D.; Smith, M.; Soldatov, A.; Soltz, R. A.; Sondheim, W. E.; Sörensen, S.; Stankus, P. W.; Starinsky, N.; Steinberg, P.; Stenlund, E.; Ster, A.; Stoll, S. P.; Sugioka, M.; Sugitate, T.; Sullivan, J. P.; Sumi, Y.; Sun, Z.; Suzuki, M.; Takagui, E. M.; Taketani, A.; Tamai, M.; Tanaka, Kazuhiro; Tanaka, Y.; Taniguchi, E.; Tannenbaum, M. J.; Tarakanov, V.; Tarasenkova, O.; Thomas, J. H.; Thomas, T. L.; Thomas, W.D.; Tian, W. D.; Tojo, J.; Torii, H.; Towell, R. S.; Trofimov, V.; Tserruya, I.; Tsuruoka, H.; Tsvetkov, A.; Tuli, S. K.; Tydesjö, H.; Tyurin, N.; Ushiroda, T.; Vanhecke, H. W.; Vasiliev, Andrey; Velissaris, C.; Velkovska, J.; Velkovsky, M.; Verhoeven, W.; Vinogradov, A.; Volkov, М. А.; Vorobyov, A. A.; Vznuzdaev, E.; Walker, James W.; Wang, H.; Wang, S.; Watanabe, Y.; White, S.; Whitus, B. R.; Wintenberg, A.L.; Witzig, C.; Wohn, F. K.; Wong-Swanson, Belinda; Woody, C. L.; Wang, Xie; Yagi, K.; Yokkaichi, S.; Young, G. R.; Yushmanov, I. E.; Zajc, W. A.; Zhang, Z.; Zhou, S.

doi:10.1016/s0375-9474(01)01347-1

Cited by 27 publications

(16 citation statements)

References 12 publications

Supporting

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“…. 92% respectively), the Pythia calculations are in perfect agreement with the (at that time preliminary) PHENIX data [25] for charged hadrons and for neutral pions in the case of peripheral collisions, as can be seen in Figs 6 and 7. We can thus conclude that our Pythia calculation with the correct extrapolation provides an accurate basis for the experimental comparison.…”

Section: Quenching By Multiple Collisions and Comparison With Datasupporting

confidence: 82%

“…As Fig. 6, but here a comparison of the present calculations with the PHENIX data[25] on π0 is depicted.…”

mentioning

confidence: 97%

“…Comparison of the calculations at midrapidity with the (at that time preliminary) PHENIX data[25] (but see also[1]) on charged hadrons for three different centralities. The thin dashed lines indicate the results from Pythia scaled with a corresponding binary collision number N coll .…”

mentioning

confidence: 98%

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Quenching of highp⊥hadron spectra by hadronic interactions in heavy ion collisions at relativistic energies

Gallmeister

Greiner

2003

Phys. Rev. C

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Typically the materialization of high energetic transverse partons to hadronic jets is assumed to occur outside the reaction zone in a relativistic heavy ion collision. In contrast, a quantum mechanical estimate yields a time on the order of only a few fm/c for building up the hadronic wavefunction for jets with typical transverse momenta of p ⊥ ≤ 10 GeV as accessible at RHIC facilities. The role of possible elastic or inelastic collisions of these high p ⊥ particles with the bulk of hadrons inside the fireball is addressed by means of an opacity expansion in the number of collisions. This analysis shows that the hadronic final state interactions can in principle account for the modification of the (moderate) high p ⊥ spectrum observed for central collisions at RHIC.

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Section: Quenching By Multiple Collisions and Comparison With Datasupporting

confidence: 82%

“…As Fig. 6, but here a comparison of the present calculations with the PHENIX data[25] on π0 is depicted.…”

mentioning

confidence: 97%

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Quenching of highp⊥hadron spectra by hadronic interactions in heavy ion collisions at relativistic energies

Gallmeister

Greiner

2003

Phys. Rev. C

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“…The observables dN ch /dη, dE T /dη, v 2 (p T ) (see Refs. 27,28,29,30 ) used to constrain the geometry experimentally are also illustrated. dence for back-to-back correlations predicted by pQCD (and checked via the PYTHIA generator).…”

Section: Introductionmentioning

confidence: 99%

Jet Quenching and Radiative Energy Loss in Dense Nuclear Matter

Gyulassy

Vitev

Wang

et al. 2004

Quark–Gluon Plasma 3

301

376

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“…At RHIC energy √ s = 500 GeV, virtually no deviations between the dipole approach and the NLO parton model have been found for y > 0.5 [7]. This means that one can safely compare the dipole approach to future DY measurements from the two PHENIX muon arms [14].…”

mentioning

confidence: 93%

Investigating the Drell-Yan transverse momentum distribution in the color dipole approach

2003

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We study the influence of unitarity corrections on the Drell-Yan transverse momentum distribution within the color dipole approach. These unitarity corrections are implemented through the multiple scattering Glauber-Mueller approach, which is contrasted with a phenomenological saturation model. The process is analyzed for the center of mass energies of the Relativistic Heavy Ion Collider (RHIC, √ s = 500GeV) and of the Large Hadron Collider (LHC, √ s = 14 TeV). In addition, the results are extrapolated down to current energies of proton-proton collisions, where non-asymptotic corrections to the dipole approach are needed. It is also shown that in the absence of saturation, the dipole approach can be related to the QCD Compton process.FIG. 1: In the target rest frame, DY dilepton production looks like a bremsstrahlung. A quark or an anti-quark from the projectile hadron scatters off the target color field (denoted by a curly line) and radiates a photon (γ * ) with mass M (before or after the quark scatters), which subsequently decays into the lepton pair (l + l − ).

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Overview of PHENIX results from the first RHIC run

Cited by 27 publications

References 12 publications

Quenching of highp⊥hadron spectra by hadronic interactions in heavy ion collisions at relativistic energies

Quenching of highp⊥hadron spectra by hadronic interactions in heavy ion collisions at relativistic energies

Jet Quenching and Radiative Energy Loss in Dense Nuclear Matter

Investigating the Drell-Yan transverse momentum distribution in the color dipole approach

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