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Ajitanand, N. N.; Aphecetche, L.; Barish, K. N.; Bathe, S.; Baublis, V.; Bennett, R.; Brown, D. S.; Bumazhnov, V.; Bunce, G.; Burward-Hoy, J. M.; Chung, P.; Constantin, P.; David, G.; Delagrange, H.; Donadelli, M.; Drees, A.; Dzhordzhadze, V.; Enokizono, A.; Espagnon, B.; Forestier, B.; Fraenkel, Z.; Fujiwara, K.; Fukao, Y.; Garishvili, I.; Gastineau, F.; Perdekamp, M. Grosse; Hachiya, T.; Henni, A. Hadj; Haegemann, C.; Haggerty, J. S.; Harada, H.; Heffner, M.; Hemmick, T. K.; Hong, B.; Hornback, D.; Imai, K.; Isupov, A.; Jia, J.; Jin, J.; Jouan, D.; Kamihara, N.; Kim, D. J.; Kinney, E.; Kiyomichi, A.; Kochenda, L.; Kotchetkov, D.; Kral, A.; Kroon, P. J.; Le Bornec, Y.; Lee, T.; Leitch, M. J.; Liu, M. X.; Makdisi, Y. I.; Malakhov, A.; McCumber, M.; Mishra, G. C.; Mishra, M.; Mitrovski, M.; Moukhanova, T. V.; Mukhopadhyay, D.; Murata, J.; Nakano, K.; Nguyen, M.; Otterlund, Ingvar; Ozawa, K.; Park, J.; Peressounko, D. Yu; Ravinovich, I.; Reuter, M.; Reygers, K.; Rosati, M.; Rukoyatkin, P.; Sakata, H.; Sato, S.; Sawada, S.; Seele, J.; Semenov, V.; Seto, R.; Shea, T. K.; Shoji, K.; Sickles, A.; Silvestre, C.; Singh, C. P.; Skutnik, S.; Soldatov, A.; Sondheim, W. E.; Sorensen, S. P.; Sziklai, J.; Tanaka, K. H.; Tannenbaum, M. J.; Tojo, J.; Tserruya, I.; Tuli, S. K.; Valle, H.; Willis, N.; Ying, J.; Yokkaichi, S.; Younus, I.; Zaudtke, O.; Zimanyi, J.
Physical review letters, 04/2007, Letnik: 98, Številka: 16Journal Article
Differential measurements of elliptic flow (v(2)) for Au+Au and Cu+Cu collisions at root s(NN)=200 GeV are used to test and validate predictions from perfect fluid hydrodynamics for scaling of v(2) with eccentricity, system size, and transverse kinetic energy (KET). For KET equivalent to m(T)-m up to similar to 1 GeV the scaling is compatible with hydrodynamic expansion of a thermalized fluid. For large values of KET mesons and baryons scale separately. Quark number scaling reveals a universal scaling of v(2) for both mesons and baryons over the full KET range for Au+Au. For Au+Au and Cu+Cu the scaling is more pronounced in terms of KET, rather than transverse momentum.
