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Adler, C.; Ahammed, Z.; Allgower, C.; Amonett, J.; Anderson, B. D.; Anderson, M.; Averichev, G. S.; Balewski, J.; Barannikova, O.; Barnby, L. S.; Baudot, J.; Bekele, S.; Belaga, V. V.; Bellwied, R.; Berger, J.; Bichsel, H.; Billmeier, A.; Bland, L. C.; Blyth, C. O.; Bonner, B. E.; Boucham, A.; Brandin, A. V.; Bravar, A.; Cadman, R. V.; Caines, H.; Sánchez, M. Calderón De La Barca; Cardenas, A.; Carroll, J. T.; Castillo, J.; Castro, M.; Cebra, D.; Chaloupka, P.; Chattopadhyay, S.; Chen, Y.; Chernenko, S.; Cherney, M.; Chikanian, A.; Choi, Bong‐Hyuk; Christie, W.; Coffin, J. P.; Cormier, T. M.; Corral, M. M.; Cramer, J. G.; Crawford, H. J.; Derevschikov, A. A.; Didenko, L.; Dietel, T.; Draper, J. E.; Dunin, V. B.; Dunlop, J. C.; Eckardt, V.; Efimov, L. G.; Емелянов, В.; Engelage, J.; Eppley, G.; Erazmus, B.; Fachini, P.; Faine, V.; Faivre, J.; Fatemi, R.; Filimonov, K.; Finch, E.; Fisyak, Y.; Flierl, D.; Foley, K. J.; Fu, J.; Gagliardi, C. A.; Gagunashvili, N.; Gans, J.; Gaudichet, L.; Germain, M.; Geurts, F. J. M.; Ghazikhanian, V.; Grachov, O.; Grigoriev, V.; Guedon, M.; Gushin, E.; Hallman, T. J.; Hardtke, D.; Harris, J. W.; Henry, T. W.; Heppelmann, S.; Herston, T.; Hippolyte, B.; Hirsch, A.; Hjort, E.; Hoffmann, G. W.; Horsley, M.; Huang, H. Z.; Humanic, T. J.; Igo, G.; Ishihara, A.; Ivanshin, Yu.; Jacobs, P.; Jacobs, W. W.; Janik, M. A.; Johnson, I.; Jones, P. G.; Judd, E. G.; Kaneta, M.; Kaplan, M.; Keane, D.; Kiryluk, J.; Kisiel, A.; Klay, J. L.; Klein, S. R.; Klyachko, A.; Kollegger, T.; Константинов, А. С.; Kopytine, M.; Kotchenda, L.; Kovalenko, A. D.; Krämer, M.; Кравцов, П.; Krueger, K.; Kuhn, C.; Куликов, А. И.; Kunde, G. J.; Kunz, C. L.; Kutuev, R.Kh.; Кузнецов, А. А.; Lakéhal-Ayat, L.; Lamont, M. A.C.; Landgraf, J. M.; Lange, S.; Lansdell, C. P.; Lasiuk, B.; Laue, F.; Lauret, J.; Lebedev, A.; Lednický, R.; Leontiev, V. M.; LeVine, M. J.; Li, Q.; Lindenbaum, S. J.; Lisa, M. A.; Liu, F.; Liu, L.; Liu, Z.; Liu, Q. J.; Ljubičić, T.; Llope, W. J.; LoCurto, G.; Long, H.; Longacre, R. S.; Lopez-Noriega, M.; Love, W. A.; Ludlam, T.; Lynn, D.; Ma, Jin; Magestro, D.; Majka, R.; Margetis, S.; Markert, C.; Martin, L.; Marx, J. N.; Matis, H. S.; Matulenko, Yu. A.; McShane, T. S.; Meißner, F.; Melnick, Yu; Meschanin, A.; Messer, M.; Miller, Michael L.; Milosevich, Z.; Minaev, N. G.; Mitchell, J. T.; Moore, C. F.; Morozov, V.; Moura, M. M. de; Munhoz, M. G.; Nelson, J. M.; Nevski, P.; Никитин, В. А.; Nogach, L. V.; Norman, B.; Nurushev, S. B.; Odyniec, G.; Ogawa, A.; Окороков, В. А.; Oldenburg, M.; Olson, D.; Paić, G.; Pandey, S. U.; Panebratsev, Y.; Panitkin, S.; Pavlinov, A. I.; Pawlak, T.; Perevoztchikov, V.; Peryt, W.; Петров, В. А.; Planinić, M.; Pluta, J.; Porile, N.; Porter, J.; Poskanzer, A. M.; Potrebenikova, E.; Prindle, D.; Pruneau, C.; Putschke, J.; Rai, G.; Rakness, G.; Ravel, O.; Ray, R. L.; Razin, S. V.; Reichhold, D.; Reid, J. G.; Renault, G.; Retière, F.; Ridiger, A.; Ritter, H. G.; Roberts, J.; Rogachevski, O. V.; Romero, J. L.; Rose, A.; Roy, C.; Rykov, V. L.; Sakrejda, I.; Salur, S.; Sandweiss, J.; Savin, I.; Schambach, J.; Scharenberg, R. P.; Schmitz, N.; Schroeder, L. S.; Schüttauf, A.; Schweda, K.; Seger, J.; Seliverstov, D. M.; Seyboth, P.; Shahaliev, E.; Shestermanov, K. E.; Shimanskii, S. S.; Simon, F.; Škoro, G.; Smirnov, N.; Snellings, Raimond; Sorensen, P.; Sowiński, J.; Spinka, H.; Srivastava, B.; Stephenson, E. J.; Stock, R.; Stolpovsky, A.; Strikhanov, M.; Stringfellow, B.; Struck, C.; Suaide, Alexandre Alarcon Do Passo; Sugarbaker, E.; Suire, C.; Šumbera, M.; Surrow, B.; Symons, T. J. M.; Toledo, A. Szanto de; Szarwas, P.; Tai, A.; Takahashi, J.; Tang, A. H.; Thein, D.; Thomas, J. H.; Thompson, M.; Tikhomirov, Vladimiro; Tokarev, M.; Tonjes, M. B.; Trainor, T. A.; Trentalange, S.; Tribble, R. E.; Trofimov, V.; Tsai, O. D.; Ullrich, T.; Underwood, D. G.; Buren, G. Van; VanderMolen, A. M.; Vasilevski, I. M.; Vasiliev, A.; Vigdor, S. E.; Voloshin, S. A.; Wang, F.; Ward, H.; Watson, J. W.; Wells, R.; Westfall, G. D.; Whitten, C.; Wieman, H.; Willson, R.; Wissink, S. W.; Witt, R.; Wood, J.; Xu, N.; Xu, Z.; Yakutin, A. E.; Yamamoto, E.; Yang, Jing; Yepes, P.; Yurevich, V. I.; Zanevski, Y. V.; Zborovský, I.; Zhang, H.; Zhang, W. M.; Zoulkarneev, R.; Zubarev, A. N.

doi:10.1103/physrevlett.90.082302

Cited by 627 publications

(100 citation statements)

References 40 publications

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“…Comparing p + p and AA collisions, one might expect some changes in particle correlations: there could be an increase in correlations due to a possible increase of jet multiplicities in AA collisions or, conversely, some decrease due to the suppression of high p T back-to-back correlations [44]. Hoever, AA collisions exhibit long η range correlations (the "ridge") [45,46], which are not seen in p + p collisions and the origin of which is under investigation [47].…”

Section: E Nonflow Contribution For Various Methodsmentioning

confidence: 99%

Charged and strange hadron elliptic flow inCu+Cucollisions atsNN=
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
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59
4
23
0
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We present the results of an elliptic flow, v 2 , analysis of Cu + Cu collisions recorded with the solenoidal tracker detector (STAR) at the BNL Relativistic Heavy Ion Collider at √ s NN = 62.4 and 200 GeV. Elliptic flow as a function of transverse momentum, v 2 (p T ), is reported for different collision centralities for charged hadrons h ± and strangeness-ontaining hadrons K 0 S , , , and φ in the midrapidity region |η| < 1.0. Significant reduction in systematic uncertainty of the measurement due to nonflow effects has been achieved by correlating particles at midrapidity, |η| < 1.0, with those at forward rapidity, 2.5 < |η| < 4.0. We also present azimuthal correlations in p + p collisions at (2010) energy, m T − m, and (ii) at intermediate p T , 2 < p T < 4 GeV/c, it scales with the number of constituent quarks, n q . We have found that ideal hydrodynamic calculations fail to reproduce the centrality dependence of v 2 (p T ) for K 0 S and . Eccentricity scaled v 2 values, v 2 /ε, are larger in more central collisions, suggesting stronger collective flow develops in more central collisions. The comparison with Au + Au collisions, which go further in density, shows that v 2 /ε depends on the system size, that is, the number of participants N part . This indicates that the ideal hydrodynamic limit is not reached in Cu + Cu collisions, presumably because the assumption of thermalization is not attained.

show abstract

Section: E Nonflow Contribution For Various Methodsmentioning

confidence: 99%

Charged and strange hadron elliptic flow inCu+Cucollisions atsNN=
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
Self Cite
59
4
23
0
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show abstract

“…A significant suppression of high-p T hadron production relative to a simple binary collision scaling from p + p has been observed at RHIC in central Au + Au collisions [1]. Furthermore, it was found that jetlike correlations opposite to trigger jets are suppressed and that the azimuthal anisotropy in hadron emission persists out to very high p T [2][3][4]. In contrast, no suppression effects were seen in d + Au collisions [5][6][7][8], which has led to the conclusion that the observations made in Au + Au are attributable to the high-density medium produced in such collisions and not to initial-state effects.…”

Section: Introductionmentioning

confidence: 91%

Inclusiveπ0,η, and direct photon production at high transverse momentum inp+p
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
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39
3
13
0
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We report a measurement of high-p T inclusive π 0 , η, and direct photon production in p + p and d + Au collisions at √ s NN = 200 GeV at midrapidity (0 < η < 1). Photons from the decay π 0 → γ γ were detected in the barrel electromagnetic calorimeter of the STAR experiment at the Relativistic Heavy Ion Collider. The η → γ γ decay was also observed and constituted the first η measurement by STAR. The first direct photon cross-section measurement by STAR is also presented; the signal was extracted statistically by subtracting the π 0 , η, and ω(782) decay background from the inclusive photon distribution observed in the calorimeter. The analysis is described in detail, and the results are found to be in good agreement with earlier measurements and with next-to-leading-order perturbative QCD calculations.

show abstract

“…It is the ratio between the measured particle spectra from Au + Au collisions normalized by the corresponding number of binary collisions and the measured spectra in elementary p + p collisions [36]. Together with the measurement of the disappearance of back-to-back high-p T hadron correlations in central Au + Au collisions attributed to interaction of the energetic jet particles with the formed medium [37], it was concluded that matter created at RHIC is highly interacting. The identified particle R AA from Au + Au collisions at 200 GeV shows that even the strange particle spectra are also suppressed, and there is a grouping of baryons and mesons with respect to their suppression in the intermediate-p T region.…”

Section: Nuclear Modification Factorsmentioning

confidence: 98%

Strange and multistrange particle production in Au + Au collisions atsNN=62.4 GeV

Aggarwal¹,

Ahammed²,

Alakhverdyants³

et al. 2011

Phys. Rev. C

Self Cite

110

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We present results on strange and multistrange particle production in Au + Au collisions at √ s NN = 62.4 GeV as measured with the STAR detector at RHIC. Midrapidity transverse momentum spectra and integrated yields of K 0 S , , , and and their antiparticles are presented for different centrality classes. The particle yields and ratios follow a smooth energy dependence. Chemical freeze-out parameters, temperature, baryon chemical potential, and strangeness saturation factor obtained from the particle yields are presented. Intermediate transverse momentum (p T ) phenomena are discussed based on the ratio of the measured baryon-to-meson spectra and nuclear modification factor. The centrality dependence of various measurements presented show a similar behavior as seen in Au + Au collisions at √ s NN = 200 GeV.

show abstract

Disappearance of Back-To-Back High-pTHadron Correlations in CentralAu+AuCollisions at
C. Adler¹,
Z. Ahammed²,
C. Allgower³
et al.

Cited by 627 publications

References 40 publications

Charged and strange hadron elliptic flow inCu+Cucollisions atsNN=
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
Self Cite
59
4
23
0
View full text Add to dashboard Cite

Charged and strange hadron elliptic flow inCu+Cucollisions atsNN=
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
Self Cite
59
4
23
0
View full text Add to dashboard Cite

Inclusiveπ0,η, and direct photon production at high transverse momentum inp+p
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
Self Cite
39
3
13
0
View full text Add to dashboard Cite

Strange and multistrange particle production in Au + Au collisions atsNN=62.4 GeV

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Disappearance of Back-To-Back High-pTHadron Correlations in CentralAu+AuCollisions atC. Adler1, Z. Ahammed2, C. Allgower3 et al.

Cited by 627 publications

References 40 publications

Charged and strange hadron elliptic flow inCu+Cucollisions atsNN=Abelev1, Aggarwal2, Ahammed3 et al. 2010Phys. Rev. CSelf Cite594230View full textAdd to dashboardCite

Charged and strange hadron elliptic flow inCu+Cucollisions atsNN=Abelev1, Aggarwal2, Ahammed3 et al. 2010Phys. Rev. CSelf Cite594230View full textAdd to dashboardCite

Inclusiveπ0,η, and direct photon production at high transverse momentum inp+pAbelev1, Aggarwal2, Ahammed3 et al. 2010Phys. Rev. CSelf Cite393130View full textAdd to dashboardCite

Strange and multistrange particle production in Au + Au collisions atsNN=62.4 GeV

Contact Info

Product

Resources

About

Disappearance of Back-To-Back High-pTHadron Correlations in CentralAu+AuCollisions at
C. Adler¹,
Z. Ahammed²,
C. Allgower³
et al.

Charged and strange hadron elliptic flow inCu+Cucollisions atsNN=
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
Self Cite
59
4
23
0
View full text Add to dashboard Cite

Charged and strange hadron elliptic flow inCu+Cucollisions atsNN=
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
Self Cite
59
4
23
0
View full text Add to dashboard Cite

Inclusiveπ0,η, and direct photon production at high transverse momentum inp+p
Abelev¹,
Aggarwal²,
Ahammed³
et al. 2010
Phys. Rev. C
Self Cite
39
3
13
0
View full text Add to dashboard Cite