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- W2555876930 abstract "In ultrarelativistic heavy ion collision the Quantum chromodynamics (QCD), the theory of the strong interaction predicts a phase transition from normal hadronic matter of confined state of quarks and gluons to a deconfined state of quarks and gluons, called Quark Gluon Plasma (QGP). Quark Gluon Plasma can be formed at high baryonic density or high temperature or at both. In heavy ion collision at RHIC and LHC energy a phase transition from confined state to a deconfined state of Quark Gluon Plasma is expected. Strangeness is one of the earliest proposed signature of QGP. Strangeness is an important tool to get information about the reaction mechanism of Heavy Ion Collision because it is produced only after collision. In QGP state strangeness could be easily produced from pair production of strange-antistrange quark-pairs. There are two basic mechanisms through which this pair production is possible, one is through fusion of two gluons and another is a light quark and a light antiquark annihilates and goes to ss-pairs. g + g → ss and q + q → ss (where q=u,d) The main interest in strange particle production in Heavy ion collision is the expectation of production rate of strangeness per nucleon will be enhanced, in comparison to elementary nucleonnucleon collision, if QGP is formed. The study of absolute yield and yield normalized with participant pair is also important. In this paper we will study the yield and normalized yield of strange particles, as a function of collision energy, in central nucleus-nucleus collision and we will compare the data [1] with result we have got from three model, HIJING, AMPT and UrQMD. RESULTS AND DISCUSSION" @default.
- W2555876930 created "2016-11-30" @default.
- W2555876930 creator A5088048393 @default.
- W2555876930 date "2013-01-01" @default.
- W2555876930 modified "2023-09-27" @default.
- W2555876930 title "Strange Particles Production in Heavy Ion Collisions" @default.
- W2555876930 hasPublicationYear "2013" @default.
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