Abstract

Based on statistical thermal approaches, the transverse momentum distribution of the well-identified produced particles, π+π^+, π−π^-, K+K^+, K−K^-, pp, pˉ\bar{p}, is studied. From the partition function of grand-canonical ensemble, we propose a generic expression for the dependence of the full chemical potential μμ on rapidity yy. Then, by fitting this expression with the experimental results of most central p⊥p_{\perp} and d2N/2πp⊥dp⊥dyd^2 N/2 πp_{\bot} dp_{\bot} dy, at 7.77.7, 11.511.5, 19.619.6, 2727, 3939, 130130, 200 200~GeV, we introduce a generic expression for the rapidity dependence of μμ, at different energies and particle types, μ=a+by2μ=a+b y^2. The resulting energy dependence reads sNN=c[(μ−a)/b]d/2\sqrt{s_{\mathtt{NN}}}=c[(μ-a)/b]^{d/2}. As a validation check, the proposed approach reproduces, excellently, the rapidity spectra measured at different energies.

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