Abstract

Within a multiphase transport model we study phi meson production in relativistic heavy ion collisions from both superposition of initial multiple proton–proton interactions and the secondary collisions in the produced hadronic matter. The yield of phi mesons is then reconstructed from their decaying product of either the kaon–antikaon pairs or the dimuon pairs. Since the kaon–antikaon pairs at midrapidity with low transverse momenta are predominantly rescattered or absorbed in the hadronic medium, they cannot be used to reconstruct the phi meson and lead thus to a smaller reconstructed phi meson yield than that reconstructed from the dimuon channel. With in-medium mass modifications of kaons and φ mesons, the φ yield from dimuons is further enhanced compared to that from the kaon–antikaon pairs. The model result is compared with the experimental data at the CERN/SPS and RHIC energies and its implications to quark–gluon plasma formation are discussed.

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