Elliptic flow of charged pions, protons and strange particles emitted in Pb plus Au collisions at top SPS energy

0385252 - ÚJF 2013 RIV NL eng J - Článek v odborném periodiku
Adamová, Dagmar - Agakishiev, G. - Andronic, A. - Antonczyk, D. - Appelshäuser, H. - Belaga, V. - Bielcikova, J. - Braun-Munzinger, P. - Busch, O. - Cherlin, A. - Damjanović, S. - Dietel, T. - Dietrich, L. - Drees, A. - Dubitzky, W. - Esumi, S. I. - Filimonov, K. - Fomenko, K. - Kushpil, Vasilij - Šumbera, Michal … celkem 52 autorů
Elliptic flow of charged pions, protons and strange particles emitted in Pb plus Au collisions at top SPS energy.
Nuclear Physics. A. Roč. 894, NOV 2012 (2012), s. 41-73. ISSN 0375-9474. E-ISSN 1873-1554
Grant CEP: GA MŠMT LA08015
Institucionální podpora: RVO:61389005
Klíčová slova: flow * strangeness * viscosity
Kód oboru RIV: BG - Jaderná, atomová a mol. fyzika, urychlovače
Impakt faktor: 1.525, rok: 2012

Differential elliptic flow spectra v(2)(p(T)) of pi(-), K-S(0), p, Lambda have been measured at root s(NN) = 17.3 GeV around midrapidity by the CERN-CERES/NA45 experiment in mid-central Pb + Au collisions (10% of sigma(geo)). The P-T range extends from about 0.1 GeV/c, (0.55 GeV/c for Lambda) to more than 2 GeV/c. Protons below 0.4 GeV/c are directly identified by dE/dx. At higher p(T), proton elliptic flow is derived as a constituent, besides pi(+) and K+, of the elliptic flow of positive pion candidates. This retrieval requires additional inputs: (i) of the particle composition, and (ii) of v(2)(p(T)) of positive pions. For (i), particle ratios obtained by NA49 are adapted to CERES conditions; for (ii), the measured v(2)(p(T)) of negative pions is substituted, assuming pi(+) and pi(-) elliptic flow magnitudes to be sufficiently close. The v(2)(p(T)) spectra are compared to ideal-hydrodynamics calculations. In synopsis of the series pi(-)-K-S(0)-p-Lambda, flow magnitudes are seen to fall with decreasing P-T progressively even below hydro calculations with early kinetic freeze-out (T-f = 160 MeV) leaving not much time for hadronic evolution. The proton v(2)(P-T) data show a downward swing towards low p(T) with excursions into negative v(2) values. The pion-flow isospin asymmetry observed recently by STAR at RHIC, invalidating in principle our working assumption, is found in its impact on proton flow bracketed from above by the direct proton flow data, and not to alter any of our conclusions. Results are discussed in perspective of recent viscous hydrodynamics studies which focus on late hadronic stages.
Trvalý link: http://hdl.handle.net/11104/0217069