In ultrarelativistic heavy-ion collisions, in the 2 GeV 6 GeV transverse momentum region, the soft and semi-hard multiple scattering of the incoming nucleons in the nuclear medium results in the broadening of the expected hadronic (e.g. pion) spectra relative to proton-proton () collisions. Thus, higher transverse-momentum regions are populated than in collisions. In a perturbative QCD based calculation we include the intrinsic transverse momentum () of the partons in the nucleon (determined from collisions), augmented by the extra broadening obtained via a systematic analysis of proton-nucleus () collisions in the energy range 17 39 AGeV. The original polynomial spectra are modified, and a nearly exponential spectrum appears in the region 2$\lesssim p_\perp\lesssim 3.5\sqrt{s}=$130 AGeV), the slope of the calculated spectra is reminiscent of that of fluid-dynamical descriptions, but lacks any thermal origin. We determine and discuss the size of the modifications originating in multiple scattering, which lead to this state of affairs.

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