期刊论文、会议论文

Csernai, L. P.

英文

Nuclear Physics A

0375-9474

2010

834

1-4

261c-264c

10th International Conference on Nucleus-Nucleus Collisions (NN2009)

AUG 16-21, 2009

Beijing, PEOPLES R CHINA

[Csernai, L. P.;Cheng, Y.;Mishustin, I. N.;Strottman, D.] Goethe Univ Frankfurt, Frankfurt Inst Adv Studies, D-60438 Frankfurt, Germany.^[Csernai, L. P.;Cheng, Y.;Magas, V. K.] Univ Bergen, Inst Phys & Technol, N-5007 Bergen, Norway.^[Csernai, L. P.] Res Inst Particle & Nucl Phys, MTA KFKI, H-1525 Budapest, Hungary.^[Cheng, Y.] Huazhong Normal Univ, Inst Particle Phys, Wuhan 430079, Peoples R China.^[Magas, V. K.] Univ Barcelona, Dept Estructura & Constituents Mat, E-08028 Barcelona, Spain.^[Mishustin, I. N.] IV Kurchatov Atom Energy Inst, Moscow 123182, Russia.^[Strottman, D.] Los Alamos Natl Lab, Div Theoret, Los Alamos, NM 87545 USA.

China Inst Atom Energy

RADARWEG 29, 1043 NX AMSTERDAM, NETHERLANDS

ELSEVIER

10.1016/j.nuclphysa.2009.12.054

本校为其他机构

The Fluid Dynamical (FD) models are considered to be a good description of heavy ion reactions with higher collision energies. Recent results indicate that the collective flow develops in the Quark Gluon Plasma (QGP) phase, what results in the Constituent Quark Number (NCQ) scaling of the flow. At the same time, between the deconfined ideal QGP and the Hadronic Matter, a so-called "Quarkyonic Matter" is predicted, where the dominant degrees of freedom are quarks. In FD model we assume the formation of the quarkyonic matter in the final Freeze O...