The formation of the quark-gluon plasma in relativistic nuclear collisions may be determined by enhanced production of φ mesons. This enhancement would result from the absence of the Okubo-Zweig-Iizuka suppression which inhibits φ production in ordinary p-p and π-p collisions, and from a large abundance of strange quarks in the plasma. The φ will not rescatter significantly in the subsequent expanding hadronic phase and would thereby retain information on the conditions of the hot plasma.
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A. Shor (1985) studied this question.
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